<?xml version="1.0"?>
<rss version="2.0"><channel><title>Cosmere Nerd Things</title><link>https://www.17thshard.com/blogs/blog/104-cosmere-nerd-things/</link><description><![CDATA[<p>
	A place for me to record my thoughts after overthinking different aspects of the cosmere.
</p>]]></description><language>en</language><item><title>Rosharan Miles (and other units of distance)</title><link>https://www.17thshard.com/blogs/entry/821-rosharan-miles-and-other-units-of-distance/</link><description><![CDATA[
<p>
	<span style="font-size:16px;"><span style="color:#e74c3c;"><strong>***** Warning: Rhythm of War spoilers below *****</strong></span></span>
</p>

<p>
	While working on some updates to our <a href="https://roshar.17thShard.com" rel="external nofollow">"Interactive Map and Timeline of Roshar"</a> I came across something that intrigued me regarding Rosharan units for distance.
</p>

<p>
	<span style="color:#e74c3c;"><strong>EDIT:</strong> I'm coming back to this a few months later because I've just received my 2021 TWoK leatherbound and, to my surprise, the scale on the Alethkar map (referenced below) <strong>is gone</strong>. That's right. The original Alethkar map had a north arrow and a scale. The 2020 TWoK leatherbounds have the north arrow removed but the scale remains. <em>Apparently</em> they made some kind of last minute change that wasn't included in the 2020 printings because in the 2021 TWoK leatherbounds both the north arrow and the scale have been removed. Weird! (there's also a white shadow behind the text on the map, making the blue font stand out much brighter--that's actually the more noticeable difference)</span>
</p>

<p>
	<span style="color:#e74c3c;">I'm leaving this entire post as-is. That scale was really the heart of my speculation below, but I'm not surprised it was apparently wrong. Turns out my first "final thought" below (<em>I think the scale on the Alethkar map is probably just an oversight, and that it's wrong...</em>) was dead on. <img alt=":)" data-emoticon="true" height="20" src="https://uploads.17thshard.com/emoticons/default_smile.png" srcset="https://uploads.17thshard.com/emoticons/smile@2x.png 2x" title=":)" width="20"> The scale was our best reference to what a Rosharan mile might be, without that there's much less substance here. </span>
</p>

<p>
	<span style="color:#e74c3c;"><em>That said,</em> I quoted a lot of references to miles in the text. So perhaps when I have some time I'll circle back and make some fresh guesses!</span>
</p>

<p>
	<u><strong>Some background info first</strong></u>
</p>

<p>
	<a contenteditable="false" data-ipshover="" data-ipshover-target="https://www.17thshard.com/profile/18198-paleo/?do=hovercard" data-mentionid="18198" href="https://www.17thshard.com/profile/18198-paleo/" id="ips_uid_1980_10" rel="" style="">@Paleo</a> was <a class="ipsAttachLink ipsAttachLink_right" href="https://en.wikipedia.org/wiki/File:Taipei_centered_azimuthal_equidistant_projection.gif" rel="external nofollow" style="float: right;"><img alt="600px-Taipei_centered_azimuthal_equidistant_projection.gif" class="ipsImage ipsImage_thumbnailed" data-fileid="44516" data-unique="l8928vl56" src="https://uploads.17thshard.com/monthly_2021_05/600px-Taipei_centered_azimuthal_equidistant_projection.gif.45b3485f31f94ed7bee2702023963879.gif" style="width: 200px; height: auto;"></a>working on a tool to measure distance on the map by clicking two points. In the process, we realized that the grid overlay we were using was not correct. <a contenteditable="false" data-ipshover="" data-ipshover-target="https://www.17thshard.com/profile/6699-otto-didact/?do=hovercard" data-mentionid="6699" href="https://www.17thshard.com/profile/6699-otto-didact/" id="ips_uid_1980_12" rel="" style="">@Otto Didact</a> was the first to realize that our world map of Roshar is a <a href="https://en.wikipedia.org/wiki/Azimuthal_equidistant_projection" rel="external nofollow">"azimuthal equidistant projection"</a>, which is an interesting globe projection where all points are at a consistently proportional distance from a chosen center point. It is perhaps best well known for it's use in the <a href="https://en.wikipedia.org/wiki/United_Nations#/media/File:Emblem_of_the_United_Nations.svg" rel="external nofollow">United Nations emblem</a>, where the North Pole is used as the center point. You don't <em>have</em> to use one of the poles as your center point, though that's the most common use. For example, the one on the right, centered on Taipei. It's a great projection to use for Roshar because the the central area of the map looks accurate, as if seen from space. The distortion is worse along the edges. Roshar conveniently has all of it's land in one corner of the globe, so the distorted parts (of the full map) are off in the middle of the sea on the other side of the planet. The map we get in the books of course is just a cropped portion of the full projection.
</p>

<p>
	<em>Anyways</em><em>...</em> We were looking into this distance measurement tool and realized the <em>calculated</em> coordinates for points toward the edges of the map didn't match up with the grid we were using. Oops! Conveniently, Oathbringer came with a <a href="https://coppermind.net/wiki/File:OB_Roshar.jpg" rel="external nofollow">beautiful map of Roshar that included the planet's grid</a>. We just need to adjust things to match this map. And come to find out not only was our <em>grid</em> wrong, but the calculations weren't quite matching the Oathbringer grid either. We never did figure out what was wrong with the grid, so we'll have to make a new one from scratch. As for the calculations, it turns out we needed to pick a better center point. It's hard to say <em>precisely</em> what the center point of the projection should be. The IDEA behind the projection, is that a great circle passing through the center coordinate will appear on the projection as a straight line. We know the center point must be on the "prime meridian" of the map, because it's the meridian that appears as a straight line, but we don't know the right latitude. I used my <a href="https://www.17thshard.com/blogs/entry/677-globe-of-roshar/" rel="">globe of Roshar</a> to draw great circles through different latitudes on the "prime meridian", and then sketched horizontal lines across the map looking for a match. Through this I found that the center point must be somewhere around 16 or 17 Rosharan degrees south of the equator. Paleo realized that 16 Rosharan degrees is the center point of the image file, so we went with that.
</p>

<p>
	<u><strong>Distance Discrepancy</strong></u>
</p>

<p>
	I've used my globe, linked above, to measure distances in the past... But I was never entirely sure of how accurate my projection for the globe was. (plus we realized the globe website wasn't quite calculating distance right through this) After working through everything above, I was quite confident with what we had. Our new grid, calculated mathematically was a pretty solid match to the one used on the Oathbringer map. We know the circumference of the planet is <a href="https://wob.coppermind.net/events/332/#e10231" rel="external nofollow">about 22,110 miles</a>. So we should have distance measurements that are as accurate as possible.
</p>

<p>
	With that done, I wanted to check something that I've always wondered about.... The <a href="https://www.brandonsanderson.com/wp-content/uploads/2019/11/twok_map-1_alethkar-webres.jpg" rel="external nofollow">Map of Alethkar</a> in The Way of Kings <em>has a scale on it</em>. So I was curious if our measurements would match this scale. I wasn't expecting it to match actually, because I've been under the impression that the scale was <em>wrong</em>. There is a new version of this same map in Oathbringer, and it has the scale removed. That has given me the impression the last few years that they were retconning some map details. Indeed, the TWoK version also includes a "North" compass heading that conflicts with the Oathbringer world map, and which the OB Alethkar map also removed. <em>Curiously</em>, however, the 10th Anniversary TWoK leatherbounds DID remove the compass but DID NOT remove the scale. So I was curious about what's going on there... Is it right or wrong? An oversight? Something else?
</p>

<p>
	One problem right off the bat is that it's not clear how the scale is meant to be used. Alethkar covers a sizeable chunk of the planet's surface, so a single linear scale can't really be <em>highly</em> accurate for the entire map. So we have to realize there's some margin of error built in. But I did find that the map of Alethkar overlays <em>quite nicely</em> onto the Oathbringer map of Roshar. From there, it was very easy to count pixels on the world map and compare them to known distances. For the azimuthal equidistant projection that we have, any line radiating from the center point as a constant scale. So given the circumference of the planet, we know the distance from the center point at 16 Rdeg South to the intersection of the prime meridian and the equator. If we count the number of pixels on the image, we have our distance/pixel relationship. Now I can draw a straight line (or line segment) at any angle through the center point, count the number of pixels to figure what the distance is. Meanwhile I can overlay the Alethkar map and count the number of pixels for the scale (in the same map). Here's what I got:
</p>

<p>
	<a class="ipsAttachLink ipsAttachLink_image" data-fileid="44517" href="//uploads.17thshard.com/monthly_2021_05/60ad3fe875cca_RosharMap.png.06f35626217c9573feac862e8e7d1774.png" rel=""><img alt="Roshar Map.png" class="ipsImage ipsImage_thumbnailed" data-fileid="44517" data-unique="f76q2p90g" src="https://uploads.17thshard.com/monthly_2021_05/60ad3fe9ca98d_RosharMap.thumb.png.e17a323f7b4c4f2e117f637046bf956c.png" style="width: 995px; height: auto;"></a>
</p>

<p>
	So the Alethkar map's scale was for a total distance of 300 units. Presumably miles. Presumably <strong><em>Rosharan miles</em></strong> I should say, because it's an in-world document, which I'll refer to as "Rmiles" from here on out for clarity. Note also my use off Rdeg for Rosharan degrees--they use 200 Rdeg in a circle.I should also note that the "22,110 mile circumference" that we have is NOT entirely clear whether that's Rosharan miles or "real" miles. I tend to get the feeling that they use real miles, internally, and so it's probably that. But we don't know. For all we know, the two are equivalent.
</p>

<p>
	Anyways, what I've done in the image above is mark 300 mile long line segments. We know these are accurate because that's simply how the projection works. And they <strong>DO NOT</strong> match the scale on the Alethkar map by a significant margin. In fact, I found the scale to be <strong>95% longer</strong>. Almost double in length. So what do we make of this?
</p>

<p>
	The very first thing I should say is that <em>this could simply be an error</em>. There are <a href="https://wob.coppermind.net/events/39/#e409" rel="external nofollow">WoBs which clearly indicate</a> that Brandon and his team had NOT entirely nailed down the details of the world map at the time The Way of Kings was written. Isaac notes in that particular one that the continent is 4000 miles across. It's currently at ~6400 miles across if measured through the center point. Depends where you measure from exactly, but it's definitely more than 4000 miles now. The scale WAS included in the leatherbound... but this could simply be an oversight. An error seems highly plausible to me.
</p>

<p>
	<u><strong>Rosharan Units of Distance</strong></u>
</p>

<p>
	But what if it's not an error? Then what do we make of this? You COULD take it as the discrepancy between "real" miles and Rosharan miles. What if the Alethkar map approximates 300 Rmiles while the segments I've drawn are just 300 real miles? Remember that the scale is... a bit ambiguous... The trick of measuring pixels like I did only works along lines radiating from the map's center point. The scale's pixel measurement that I did is not <em>quite</em> a radial line segment, and any measurements on the Alethkar map that are perpendicular to these radial lines will vary in consistency from left to right. That is to say, the scale of vertical measurements distorts as you move across the page from left to right. Where does the 300 mile scale apply? Unclear. But the margin of error shouldn't be SO far off. I'd be surprised if it's more than +/- 5%.
</p>

<p>
	So let's run with this notion that Rosharan miles are about 1.95 times the length of a real mile...
</p>

<p>
	1 Rmile = 1.95 miles = 1.95 x 5280 feet = 10,296 feet.
</p>

<p>
	I can't help but notice how close this is to a metric-like multiple of 10 as we would expect from Rosharans. Indeed, we know that they use <a href="https://wob.coppermind.net/events/115/#e1566" rel="external nofollow">ten inches per foot</a>. Or rather, I should say they use 10 Rinches per Rfoot. And for the number of feet per mile we're really more interested in Rfeet per Rmile. BUT we know that Rosharan feet are just a BIT longer than real feet, and Brandon's use of the word isn't meant to imply something highly unintuitive. This is pretty straight forward though. If we imagine 10,000 Rfeet per Rmile we get:
</p>

<p>
	1 Rmile = 1.95 miles = 1.95 x 5280 feet = 10,296 feet = 10,000 Rfeet
</p>

<p>
	1 Rfoot = 1.03 feet = 12.36 inches = 10 Rinches
</p>

<p>
	1 Rinch = 1.24 inches
</p>

<p>
	In Khriss's essay on Roshar she DOES say that their units of measurement are larger than the cosmere standard equivalent units. And with these assumptions it's precisely what we get. Miles that are about twice as long as "normal". Feet that are perhaps something like 5% longer than "normal". (which matches this <a href="https://wob.coppermind.net/events/374/#e12138" rel="external nofollow">WoB</a>--5% on top of 6'-4" adds 4 inches) Inches that are ~25% longer than "normal". (emphasizing once again that this is all very approximate, based on me measuring pixels on a world map... There's room for some variance.
</p>

<p>
	<u><strong>Textual Issues</strong></u>
</p>

<p>
	Unfortunately, there are a few references in the text that conflict a bit with this interpretation. BUT there is one that, in my opinion, affirms it. And it's possible that these references could be adjusted in future leatherbound versions as none of them are in TWoK.
</p>

<blockquote class="ipsQuote" data-ipsquote="">
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		<p>
			<strong>TWoK Interlude I-1</strong>
		</p>

		<p>
			The Purelake extended in all directions, hundreds of miles wide, its glassy surface perfectly transparent.
		</p>
	</div>
</blockquote>

<p>
	The Purelake is a little over 1000 miles across and 400 miles wide. For 2X long Rmiles, that would be 500 and 200, so this fits nicely.
</p>

<blockquote class="ipsQuote" data-ipsquote="">
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		<p>
			<strong>WoR 69</strong>
		</p>

		<p>
			“Actually, I’m wondering how the trunk of a stumpweight tree got here,” she confessed. “They can’t possibly be native to this area of the Shattered Plains. Too cold out here. It might have grown along the coast, but a highstorm really carried it that far? Four hundred miles?”
		</p>
	</div>
</blockquote>

<p>
	For 2X Rmiles, it looks like the eastern coast is only 150 Rmiles away. Could say Shallan's sense of geography is off... but with her photographic memory I think this is pretty unlikely.
</p>

<blockquote class="ipsQuote" data-ipsquote="">
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		<p>
			<strong>OB 5</strong>
		</p>

		<p>
			Perhaps he could have flown all the way to Hearthstone if he'd been more practiced with his powers. As it was, he’d traveled over a thousand miles in half a day, but this last bit—ninety or so miles—had taken an excruciating three days.
		</p>
	</div>
</blockquote>

<p>
	The distance from Narak to "not quite Hearthstone" looks to be about 1700 miles. That would only be about 850 Rmiles. Though maybe Kaladin's judge of distance just isn't quite right. Or maybe with error it's just barely over 1000 Rmiles.
</p>

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		<p>
			<strong>OB 55</strong>
		</p>

		<p>
			Soon after he left through the Oathgate, everyone would slowly start to lose their powers. They’d be gone in an hour or two. Kaladin had to be relatively near—Sigzil had placed their maximum distance from him at around fifty miles, though their abilities started to fade somewhere around thirty miles.
		</p>
	</div>
</blockquote>

<p>
	This one actually AFFIRMS the idea of 2X Rmiles in my opinion.
</p>

<p>
	I'm measuring the diameter of the Shattered Plains as about 170... The exact edges aren't clear, so it depends where you measure from. But it's definitely over 150 miles. That means the radius is 75 miles minimum. In the Words of Radiance finale, we see Lopen's arm heal back in the warcamps while Kaladin is presumably <em>somewhere</em> around Narak. Lopen was easily more than 50 miles away, and certainly more than the 30-mile limit where their powers supposedly diminish.
</p>

<p>
	But for 2X Rmiles, the Shattered Plains has a radius of perhaps about 40 Rmiles, give or take. That fits MUCH better with Lopen's healing. I'd go so far as to say that if this "theory" about Rosharan miles is wrong, this reference is an error.
</p>

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		<p>
			<strong>OB 64</strong>
		</p>

		<p>
			“If you’ll all excuse me, I have to prepare for an appointment with an emperor a thousand miles away.”
		</p>
	</div>
</blockquote>

<p>
	This is Dalinar going to visit Azir.
</p>

<p>
	Azir is less than 800 miles from Urithiru, so he's just plain wrong about that distance regardless. Though I suppose overestimating 800 miles would be more reasonable than for him to say "a thousand" when it's only ~400.
</p>

<blockquote class="ipsQuote" data-ipsquote="">
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		<p>
			<strong>OB 83</strong>
		</p>

		<p>
			“The Shattered Plains ?” Yokska asked, aghast. “But Brightlord, that’s hundreds and hundreds of miles!”
		</p>
	</div>
</blockquote>

<p>
	This is correct either way.
</p>

<blockquote class="ipsQuote" data-ipsquote="">
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		<p>
			<strong>OB 93</strong>
		</p>

		<p>
			“I didn’t know of those until Kal told me about them. I used a portal between realms. Cultivation’s Perpendicularity, they call it. On your side, it’s in the Horneater Peaks.”
		</p>

		<p>
			“That’s hundreds of miles from here,” Adolin said.
		</p>
	</div>
</blockquote>

<p>
	This is correct either way. (spoken from Shadesmar in the vicinity of Kholinar)
</p>

<blockquote class="ipsQuote" data-ipsquote="">
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		<p>
			<strong>OB 108</strong>
		</p>

		<p>
			He looked back at her map and pointed. “Thaylen City,” he said. “If we continue this direction, we’ll eventually pass just north of it.”
		</p>

		<p>
			“ ‘Just north’ in this case meaning more than three hundred miles away from it, in the middle of a bead ocean.”
		</p>

		<p>
			[...]
		</p>

		<p>
			And the fact that they had to somehow escape from a ship in the middle of a sea of beads, reach the shore, then hike two hundred miles to reach Thaylen City.
		</p>
	</div>
</blockquote>

<p>
	These distances seem to refer to real miles. The distance from Thaylen City to the coast of the bead ocean where they landed is <em>about </em>200-300 miles. So this doesn't jive with 2X Rmiles.
</p>

<blockquote class="ipsQuote" data-ipsquote="">
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		<p>
			<strong>DS 1</strong>
		</p>

		<p>
			Seeing him left her speechless. He lived thousands of miles away from her. How was he here? She stammered, searching for what to say.
		</p>
	</div>
</blockquote>

<p>
	Reshi Isles is thousands of miles either way... Well, for 2X Rmiles it's not quite 2000 miles I think, but seems reasonable enough for her to say.
</p>

<blockquote class="ipsQuote" data-ipsquote="">
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			<strong>RoW 3</strong>
		</p>

		<p>
			Flying. It had worked. Not just in maneuvers and tests on the Shattered Plains, but on a real mission, flying hundreds of miles.
		</p>
	</div>
</blockquote>

<p>
	Works either way.
</p>

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		<p>
			<strong>RoW 27</strong>
		</p>

		<p>
			A thousand men at a time stood for their turn at the Oathgate, where Radiants transferred them to Azir. With a flash—a ring of light rising around the plateau—both men and banners were off, sent hundreds of miles in a heartbeat.
		</p>
	</div>
</blockquote>

<p>
	Works either way.
</p>

<blockquote class="ipsQuote" data-ipsquote="">
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		<p>
			<strong>RoW 111</strong>
		</p>

		<p>
			He was flying. Covering a hundred miles in less than half an hour.
		</p>
	</div>
</blockquote>

<p>
	This is Dalinar flying from their base in Emul to Ishar. It's not <em>entirely</em> clear where teir base was (or precisely where Ishar was). I think this works either way though, eyeballing the area.
</p>

<p>
	<u><strong>Final Thoughts</strong></u>
</p>

<p>
	I think the scale on the Alethkar map is <em>probably </em>just an oversight, and that it's wrong...
</p>

<p>
	BUT I really like this idea for the units. I think it's safe to assume that a Rosharan foot must be <em>similar</em> in length to a foot. If Rosharan miles are supposed to be closer in length to miles, there's not a great way for Rmiles to be a 10X power of Rfeet. Again, assuming feet are fairly similar, using 1000 Rfeet per Rmile gives an unreasonably short Rmile. I think the best alternative idea is that they use 5000 Rfeet per Rmile. That means you just need Rfeet at 6% longer than a real foot to give Rmiles the length of miles. Increasing the foot size a bit more gives Rmiles a bit longer as well. Using a multiple of 5 like this has precedence in their units. We know that there are 50 Rosharan minutes in a Rosharan hour, rather than 100. So this seems reasonable... But using 10,000 Rfeet per Rmile is a really nice alternative that seems to fit with the scale on the Alethkar map!
</p>

<p>
	That said, there ARE definitely some quotes (mostly in Oathbringer) that would need some revisions if this is the intent. (and one that needs to be revised if it's <em>not</em>)
</p>
]]></description><guid isPermaLink="false">821</guid><pubDate>Tue, 25 May 2021 19:49:00 +0000</pubDate></item><item><title>Stormlight Archive Timeline (v2.4.12)</title><link>https://www.17thshard.com/blogs/entry/791-stormlight-archive-timeline-v2412/</link><description><![CDATA[
<p>
	Small updates to the timeline published tonight: <a href="https://docs.google.com/spreadsheets/d/1zq5bJoKE83ggDCjH43i1hZi0CIpB2iAx7v37zQPVFK0/edit#gid=856252766" ipsnoembed="true" rel="external nofollow">https://docs.google.com/spreadsheets/d/1zq5bJoKE83ggDCjH43i1hZi0CIpB2iAx7v37zQPVFK0/edit#gid=856252766</a>
</p>

<p>
	<span data-sheets-formula-bar-text-style="font-size:13px;color:#000000;font-weight:normal;text-decoration:none;font-family:'Arial';font-style:normal;text-decoration-skip-ink:none;"><strong>Changelog:</strong></span>
</p>

<ul>
	<li>
		<span data-sheets-formula-bar-text-style="font-size:13px;color:#000000;font-weight:normal;text-decoration:none;font-family:'Arial';font-style:normal;text-decoration-skip-ink:none;">Added crude spoiler filter for References sheet. (So if you set the book filter on the Timeline sheet it will hide the events here as well. But note that it's not discriminatory about where sources come from, so people picky about spoilers should not rely on this.)</span><br>
		 
	</li>
	<li>
		<span data-sheets-formula-bar-text-style="font-size:13px;color:#000000;font-weight:normal;text-decoration:none;font-family:'Arial';font-style:normal;text-decoration-skip-ink:none;">Updated Instructions sheet. </span><br>
		 
	</li>
	<li>
		<span data-sheets-formula-bar-text-style="font-size:13px;color:#000000;font-weight:normal;text-decoration:none;font-family:'Arial';font-style:normal;text-decoration-skip-ink:none;">Fixed bug with calculation on multi-interval events. These are generally events which don't have a clear date... but I know they happen before one thing and after another. Rather than setting some manual value to place it between the two, I reference both events and have my database put it in the middle of the two. That way, if one of them gets altered later the dependent event will shift accordingly. My placement of the date previously took some of the error ranges into account, but I ran into an odd case where lopsided error and a small difference between the two referenced events was causing the "middle" event to be placed before the first. Whoops. It now just averages the two reference dates and lets the error fill in as needed on either side.</span><br>
		 
	</li>
	<li>
		<span data-sheets-formula-bar-text-style="font-size:13px;color:#000000;font-weight:normal;text-decoration:none;font-family:'Arial';font-style:normal;text-decoration-skip-ink:none;">Fixed discrepancy with Dalinar and Taravangian's visits to the Valley. This is a tricky one, and the most interesting change I've made. The previous version had some weird issues regarding these events. It involves RoW spoilers:</span>
		<div class="ipsSpoiler" data-ipsspoiler="">
			<div class="ipsSpoiler_header">
				<span>Spoiler</span>
			</div>

			<div class="ipsSpoiler_contents">
				<p>
					In Taravangian's first interlude in RoW he mentions that the "day of brilliance" was "seven years gone". I took this to mean it happened "over 7 years ago". Unfortunately this not only placed the event before my previously assumed Taravangian-Nightwatcher visit, but it also put the Diagram's creation before Dalinar visited the Valley. So... wrong because he needed to see Cultivation first, and wrong because we know Dalinar was the first human to get a visit from Cultivation in centuries. (according to her, during his visit)
				</p>

				<p>
					I first decided that my previous assumption for Taravangian was wrong. It was based on an Oathbringer ch 34 quote about Taravangian having a strange illness 5 years back. I loosely tied this to his visit to the Valley. I've now decided it probably refers to the time after the creation of the Diagram. (He was probably in seclusion for a bit as they figured out what to do with the Diagram and how to deal with Taravangian's condition moving forward.) It also fits (barely) with the next assumption I made...
				</p>

				<p>
					...Which was that "seven years gone" can reasonably mean as little as 6.5 years. So if you take the "five years ago" reference as 5.5 years and the "seven years ago" reference as 6.5 years, there's just BARELY some overlap. I'm not sure what the official timeline has to say about all of this, but I'm going to assume the Diagram was created in that little window. That's my best guess.
				</p>

				<p>
					I also bumped the date of Dalinar's visit 2.5 months earlier, keeping it within the range of error I had allowed. (The event was "5.5 years ago" from the end of Oathbringer, so I've shifted it to be 5.75 years ago, with error adjusted to allow no more than that and as little as 5.25 years ago.) There were two reasons for this. The first is that I had is visit just a few weeks prior to the creation of the Diagram, and that just plain doesn't look right. The logic of the numbers makes sense, and the error ranges allowed more reasonable dates... but it just <em>looks wrong</em> on the timeline. Dalinar had to have visited earlier (and the Diagram was maybe created just a bit later). Adding to this, however, was the Eshonai flashback marking the arrival of the Alethi on the Shattered Plains. They arrive at the end of 1168 month 4 according to that flashback. And that's a good bit of time. Four whole months to gather their armies and march to the Shattered Plains (which are NOT very far from Alethkar) seems very reasonable. Dalinar was SUPPOSED to be arriving before the main armies (before his fake hold-up). There's no way he didn't make it to the Valley until <em>month 7</em> of that year. The rest of the Alethi wouldn't just be wondering why Dalinar got held up. They'd be wondering if he was still alive. <img alt=":rolleyes:" data-emoticon="true" src="https://uploads.17thshard.com/emoticons/default_rolleyes.gif" title=":rolleyes:"> Shifting his visit back to month 5 still seems a little odd, but it's <em>better</em> at least.
				</p>
			</div>
		</div>
	</li>
	<li>
		<span data-sheets-formula-bar-text-style="font-size:13px;color:#000000;font-weight:normal;text-decoration:none;font-family:'Arial';font-style:normal;text-decoration-skip-ink:none;">Fixed Cord's birthday. I had placed her a bit older according to a Dawnshard quote, but someone noted that Oathbringer sneakily puts her as about 16.</span><br>
		 
	</li>
	<li>
		<span data-sheets-formula-bar-text-style="font-size:13px;color:#000000;font-weight:normal;text-decoration:none;font-family:'Arial';font-style:normal;text-decoration-skip-ink:none;">Added Gift's birthday. Someone else noted that Gift and Cord are twins, so knowing one birthday also gives the other's. </span><br>
		 
	</li>
	<li>
		<span data-sheets-formula-bar-text-style="font-size:13px;color:#000000;font-weight:normal;text-decoration:none;font-family:'Arial';font-style:normal;text-decoration-skip-ink:none;">Removed an event placing the Dawnshard finale in early 1175. Dawnshard happens late in 1174, so I think this is a very clear error. Probably a consequence of Dawnshard being written after RoW. I've added to the typo thread in case Dragonsteel missed it: </span><a href="https://www.17thshard.com/topic/93207-rhythm-of-war-typo-thread/?do=findComment&amp;comment=1198400" ipsnoembed="true" rel="">https://www.17thshard.com/forum/topic/93207-rhythm-of-war-typo-thread/?do=findComment&amp;comment=1198400</a><br>
		 
	</li>
	<li>
		Removed a duplicate event from RoW. Interlude I-2 was showing up twice, on separate dates. I worked through the references I had and picked the better ones to leave just one event.<br>
		 
	</li>
	<li>
		Aaaaaand... probably some other small stuff that I forgot to make a record of. <img alt=";)" data-emoticon="true" height="20" src="https://uploads.17thshard.com/emoticons/default_wink.png" srcset="https://uploads.17thshard.com/emoticons/wink@2x.png 2x" title=";)" width="20">
	</li>
</ul>
]]></description><guid isPermaLink="false">791</guid><pubDate>Wed, 24 Feb 2021 06:41:16 +0000</pubDate></item><item><title>Rhythm of War Statistical Analysis</title><link>https://www.17thshard.com/blogs/entry/760-rhythm-of-war-statistical-analysis/</link><description><![CDATA[
<p>
	I took the time to update the <a href="https://coppermind.net/wiki/Rhythm_of_War/Statistical_analysis" rel="external nofollow">statistical analysis of Rhythm of War</a> today and wanted to share some fun charts!
</p>

<p>
	SPOILERS FOR RHYTHM OF WAR!
</p>

<p>
	<strong>Word Count by Character</strong><br>
	Self explanatory. Kaladin, Shallan, and Dalinar lead the pack in that order, as I think most people would assume.
</p>

<p>
	<a class="ipsAttachLink ipsAttachLink_image" data-extension="core_Attachment" data-fileid="39858" href="//uploads.17thshard.com/monthly_2020_11/5fbc6a9fef634_2020-11-2320_46_39-StormlightAnalysis.xlsx-Excel.png.00af7607f9ed25b8ee9fd4623627003b.png" rel=""><img alt="2020-11-23 20_46_39-Stormlight Analysis.xlsx - Excel.png" class="ipsImage ipsImage_thumbnailed" data-extension="core_Attachment" data-fileid="39858" data-unique="h93knwl7z" src="https://uploads.17thshard.com/monthly_2020_11/5fbc6aa1d987e_2020-11-2320_46_39-StormlightAnalysis.xlsx-Excel.thumb.png.8374d7950a9eaca0a7f0a76233c5310d.png"></a>
</p>

<p>
	<strong>Word Count by Character (excluding the big 3)</strong><br>
	Zooming in a bit better on all the characters <em>besides</em> Kaladin, Shallan and Dalinar... Navani and Venli both leaped up tremendously in Rhythm of War. Adolin kept his title as top secondary character though, with his biggest word count yet. Lezian is the newest character with smallest word count. I guess I should also note that this has the numbers from Dawnshard as well, so you can see how high that pulled Rysn and Lopen.
</p>

<p>
	<a class="ipsAttachLink ipsAttachLink_image" data-fileid="39871" href="//uploads.17thshard.com/monthly_2020_11/5fbc8f2b86996_2020-11-2323_41_51-StormlightAnalysis.xlsx-Excel.png.66cf932b74dbb413092e10f7f8412b78.png" rel=""><img alt="2020-11-23 23_41_51-Stormlight Analysis.xlsx - Excel.png" class="ipsImage ipsImage_thumbnailed" data-fileid="39871" data-unique="jckr6sc2n" src="https://uploads.17thshard.com/monthly_2020_11/5fbc8f2d4a94a_2020-11-2323_41_51-StormlightAnalysis.xlsx-Excel.thumb.png.b5ed33feacf9ac799093b1cf24392510.png" style=""></a>
</p>

<p>
	<strong>Big Three Word Count by Book</strong><br>
	Turning attention back to the three main characters, here's how their word counts stack up for each book. Kaladin had a bit more than OB and Dalinar barely squeaked by with more words than WoR. Rhythm of War was Shallan's lowest word count yet (barely). On the whole, you can really see how Navani, Venli, and Adolin dug into their usual numbers (overall) this book.
</p>

<p>
	<img alt="2020-11-23 20_51_02-Stormlight Analysis.xlsx - Excel.png" class="ipsImage ipsImage_thumbnailed" data-fileid="39909" data-unique="ban9dznkx" src="https://uploads.17thshard.com/monthly_2020_11/5fbde13abb4fa_2020-11-2320_51_02-StormlightAnalysis.xlsx-Excel.png.a2627241ac058595dc8e5463a32e4d33.png" style="">
</p>

<p>
	<strong>Flashback Word Counts</strong><br>
	Here's how the flashbacks have gone so far. This is JUST word counts of these characters' flashback sequences. (Always surprises me how little word count Shallan's flashbacks got in WoR. Brandon packed so much punch in those for me.) Individually Eshonai and Venli would be the lowest. But together they give Rhythm of War the 3rd highest word count on flashbacks.
</p>

<p>
	<img alt="2020-11-23 20_55_05-Stormlight Analysis.xlsx - Excel.png" class="ipsImage ipsImage_thumbnailed" data-fileid="39912" data-unique="nhqsus55p" src="https://uploads.17thshard.com/monthly_2020_11/5fbde13bebb2a_2020-11-2320_55_05-StormlightAnalysis.xlsx-Excel.png.f628bfc777437dc9492e964665320944.png" style="">
</p>

<p>
	<strong>Rhythm of War Word Count by Character</strong><br>
	Here's the word counts for each character looking only at Rhythm of War. Kaladin led the pack, but only by a little. Navani had more than Venli and Eshonai combined.
</p>

<p>
	<img alt="2020-11-23 20_50_03-Stormlight Analysis.xlsx - Excel.png" class="ipsImage ipsImage_thumbnailed" data-fileid="39908" data-unique="hrfgkct6b" src="https://uploads.17thshard.com/monthly_2020_11/5fbde13a470f1_2020-11-2320_50_03-StormlightAnalysis.xlsx-Excel.png.2705e8978365e8f10f6d8a49aef570b7.png" style="">
</p>

<p>
	<strong>Word Count by Book Part</strong>
</p>

<p>
	Here's how RoW's word count is distributed among each part compared to the other books.
</p>

<p>
	<img alt="2020-11-23 20_55_42-Stormlight Analysis.xlsx - Excel.png" class="ipsImage ipsImage_thumbnailed" data-fileid="39913" data-unique="yp2qkrz0t" src="https://uploads.17thshard.com/monthly_2020_11/5fbde13c63a5d_2020-11-2320_55_42-StormlightAnalysis.xlsx-Excel.png.4605b79e308f7dae6a28f4f8091425b3.png" style="">
</p>

<p>
	<strong>Word Count by Location</strong><br>
	One thing not captured on the statistical analysis pages on Coppermind is that I've done my best to note where everyone's PoV happens.This admittedly gets a bit arbitrary... But whatever. <img alt=":)" data-emoticon="true" height="20" src="https://uploads.17thshard.com/emoticons/default_smile.png" srcset="https://uploads.17thshard.com/emoticons/smile@2x.png 2x" title=":)" width="20"> Nothing particularly exciting or notable about this graph, but here it is.
</p>

<p>
	<img alt="2020-11-23 20_52_20-Stormlight Analysis.xlsx - Excel.png" class="ipsImage ipsImage_thumbnailed" data-fileid="39910" data-unique="tcin513z7" src="https://uploads.17thshard.com/monthly_2020_11/5fbde13b2966a_2020-11-2320_52_20-StormlightAnalysis.xlsx-Excel.png.2e410ad740e66ec64aa775a23505ae6f.png" style="">
</p>

<p>
	<strong>Rhythm of War Word Count by Location</strong>
</p>

<p>
	And here's just the RoW data. I think the time in Tukar was just that one Dalinar chapter. And I think the "unknown" is Lezian when he wakes up? Seems like it didn't give any clear indication where he was there.
</p>

<p>
	<a class="ipsAttachLink ipsAttachLink_image" href="//uploads.17thshard.com/monthly_2020_11/5fbde13b8913c_2020-11-2320_54_48-StormlightAnalysis.xlsx-Excel.png.32cd4b135cdd57dcb4e9e1528b9525f4.png" data-fileid="39911" rel=""><img alt="2020-11-23 20_54_48-Stormlight Analysis.xlsx - Excel.png" class="ipsImage ipsImage_thumbnailed" data-fileid="39911" src="https://uploads.17thshard.com/monthly_2020_11/5fbde13b8913c_2020-11-2320_54_48-StormlightAnalysis.xlsx-Excel.png.32cd4b135cdd57dcb4e9e1528b9525f4.png"></a>
</p>

<p>
	<strong>Word Count by Gender</strong><br>
	This is a breakdown of PoV character gender (in terms of word count) for the entire series...
</p>

<p>
	<img alt="2020-11-23 21_01_55-Stormlight Analysis.xlsx - Excel.png" class="ipsImage ipsImage_thumbnailed" data-fileid="39914" data-unique="qiatryxrn" src="https://uploads.17thshard.com/monthly_2020_11/5fbde13cc4be2_2020-11-2321_01_55-StormlightAnalysis.xlsx-Excel.png.c0c95efdcc36be83b10d1e8d199ecf68.png" style="">
</p>

<p>
	<strong>Rhythm of War Word Count by Gender</strong><br>
	And here's the same thing but only with Rhythm of War numbers. Girl power running the show in RoW.
</p>

<p>
	<img alt="2020-11-23 21_02_12-Stormlight Analysis.xlsx - Excel.png" class="ipsImage ipsImage_thumbnailed" data-fileid="39915" data-unique="wtaonh8wd" src="https://uploads.17thshard.com/monthly_2020_11/5fbde13d34172_2020-11-2321_02_12-StormlightAnalysis.xlsx-Excel.png.332bf88e1831f22c349b02d1a229800f.png" style="">
</p>

<p>
	<strong>Chapter Word Count Distribution</strong><br>
	Okay, these last two aren't super exciting. This is a distribution of chapters over different word count ranges, so it gives you an idea of how long the chapters tend to be. Hard to see much of a trend with these ranges... But it's a pain to tinker with the range. Nothing particularly notable about this compared to other books so far I think.
</p>

<p>
	<img alt="2020-11-23 21_03_40-Stormlight Analysis.xlsx - Excel.png" class="ipsImage ipsImage_thumbnailed" data-fileid="39917" data-unique="xz34qy0si" src="https://uploads.17thshard.com/monthly_2020_11/5fbde13e16eb1_2020-11-2321_03_40-StormlightAnalysis.xlsx-Excel.png.f7c0328f3a9746d1d441248052665dfd.png" style="">
</p>

<p>
	<strong>PoV Word Count Distribution</strong><br>
	Same idea here, just breaking it down by PoV instead of chapters. The short snippy PoVs during "avalanches" brings things down.
</p>

<p>
	<img alt="2020-11-23 21_03_26-Stormlight Analysis.xlsx - Excel.png" class="ipsImage ipsImage_thumbnailed" data-fileid="39916" data-unique="btlivmm9r" src="https://uploads.17thshard.com/monthly_2020_11/5fbde13da095f_2020-11-2321_03_26-StormlightAnalysis.xlsx-Excel.png.3e6f742a746f4c18e5427fe3fe975e37.png" style="">
</p>
]]></description><guid isPermaLink="false">760</guid><pubDate>Tue, 24 Nov 2020 04:53:00 +0000</pubDate></item><item><title>Stormlight Archive Timeline (v2.4.11)</title><link>https://www.17thshard.com/blogs/entry/758-stormlight-archive-timeline-v2411/</link><description><![CDATA[
<p>
	I've updated my timeline for Dawnshard and Rhythm of War!
</p>

<p>
	<a href="https://docs.google.com/spreadsheets/d/1zq5bJoKE83ggDCjH43i1hZi0CIpB2iAx7v37zQPVFK0/edit" ipsnoembed="true" rel="external nofollow">https://docs.google.com/spreadsheets/d/1zq5bJoKE83ggDCjH43i1hZi0CIpB2iAx7v37zQPVFK0/edit</a>
</p>

<p>
	<span style="font-size:18px;"><strong>Dawnshard and RoW spoiler below!</strong></span>
</p>

<p>
	Dawnshard's timeline is fairly loose. The middle of their voyage was 6 months after OB, based on Rysn's conversation with Vstim in chapter 9. Nailing down the beginning date of the story involves a long trail of events back through Rysn's interlude, when Szeth became a Truthless, and when Gavilar was murdered.... Basically... Rysn says her accident was 2 years prior. We have a rough idea of how much time passed from Rysn's accident and her TWoK interlude. The TWoK interlude gives an idea of how long ago Szeth became Truthless. And in one TWoK Szeth interlude he connects how long ago he became Truthless with how long ago he assassinated Gavilar. The problem I found is that these don't all fit together super great. You have to make a lot of skewed assumptions in their phrasing, and then squint a little. But there's nothing WRONG, so we'll go with it. The ending is presumably an equal number of days after chapter 9 as the beginning of the voyage is prior. This is a little awkward though because the very next string of events is after they arrive in Aimia, meaning Rysn figured out Nikli was the spy... and then sat on that knowledge for several weeks without doing anything. *shrug* It also means the whole voyage took more than a month when the implications earlier suggested less. ("weeks") But again, nothing explicitly contradictory in the text, so I've run with it.
</p>

<p>
	(I also have a small gripe about how long it took them to travel from Thaylen City to the Hexi. Feels like their ship is moving WAY slower than previous ships we've seen in the books. But oh well.)
</p>

<p>
	Rhythm of War's timeline is mostly tied down to the very clear date given at the end of the book. There are two major soft spots in the primary timeline. First is that it's a little unclear how much time passes between the destruction of the 3rd node and the finale. There's several vague references that seem to mesh together though. The timeline in the middle of the story is very solid. Most of Part 1 is also very solid, but it's not clear exactly when it all occurs relative to the attack on the tower (and thus into Part 2). My solution was to base it on Everstorm timings, so I'm pretty sure the Part 1 events are accurate within +/-9 days. (less than that and the events don't fit, more and there's an awkward additional 2 weeks where nothing happens.) Shallan and Adolin have a few chapters in the middle, where they arrive at Lasting Integrity, that aren't entirely clear. I'm also just <em>assuming</em> that their last chapter is the same day as everyone else's last chapter. (there's a clue suggesting the tower occupation is over, so that makes sense) Dalinar and Jasnah's timeline is somewhat hazy... but there's not a whole lot of time spent with them, so I've just put those in as best I can and they're probably not toooo far off.
</p>

<p>
	If you spot errors of any kind let me know!
</p>
]]></description><guid isPermaLink="false">758</guid><pubDate>Thu, 19 Nov 2020 06:59:47 +0000</pubDate></item><item><title>Rosharan Spheres to US Dollars</title><link>https://www.17thshard.com/blogs/entry/693-rosharan-spheres-to-us-dollars/</link><description><![CDATA[
<p class="_1qeIAgB0cPwnLhDF9XSiJM">
	<a href="https://www.reddit.com/user/Aradanftw/" rel="external nofollow">u/Aradanftw</a> on Reddit put together <a href="https://www.reddit.com/r/Stormlight_Archive/comments/e8y8yl/spheres_to_us_dollar_currency_comparison/" rel="external nofollow">a post converting Roshar's spheres to US Dollars</a>. So this is 99% their work and not my own! But I thought it was interesting and something that I might want to reference more often down the road. Perhaps I'll remember to add more things to it.
</p>

<p class="_1qeIAgB0cPwnLhDF9XSiJM">
	My main "contribution" was a push to reduce the values by an order of magnitude. The diamond chip was originally set at $2, based on the price of a loaf of bread. I'm not sure Aradanftw was entirely on board with this opinion, but the prices I've posted below are 1/10th of that. I'll admit that I'm not great with economics and inflation values, so I'm happy to be corrected on this. But it seems to me like we should compare the prices to Earth prices <em>at a similar level of technological development</em>? So I'm thinking we should look more at 19th century (-ish) US dollars rather than 21st century US dollars? The price of bread in early/pre-industrial society is different than modern society. Even now you can go to non-Western developing countries where a bit of bread is going to be a lot less than $2. And, admittedly, part of the drive for this is that $2 as you SMALLEST denomination of currency seems off to me.
</p>

<div data-role="contentPage">
	<p class="_1qeIAgB0cPwnLhDF9XSiJM">
		Aside from that price shift, I've also reorganized everything from lowest value to highest, and reworked some of the details. So assuming 1 diamond chip = a loaf of bread = $0.20, we've got the following prices:
	</p>

	<hr data-role="contentPageBreak">
</div>

<p class="_1qeIAgB0cPwnLhDF9XSiJM">
	<u>Rosharan spheres to US Dollars:</u>
</p>

<ul>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		1 diamond chip (smallest denomination) - $0.20
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Apothecary bandages, per armlength (1 diamond chip) - $0.20
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Candied fruit (1 diamond chip) - $0.20
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Shallan's trip to the Palanaeum (2 diamond chips) - $0.40<br>
		 
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Bridgeman slave daily wages (1 diamond mark) - $1
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Bridgeman daily wages (2 diamond marks) - $2
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Tozbek's sailors' daily wages (1 ruby chip) - $2
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		<span class="_2v4IIjPhKL0PDaWaWtjJ1E _2v4IIjPhKL0PDaWaWtjJ1E _15VS32zBYFUDI5ssldQhEK"><span class="_3mIYu0jAt23sIWGr4pFcI">Shallan's slaves' daily wages (1 ruby chip + 5 ruby chips toward slave debt) - $2 + $10 toward slave debt</span></span>
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Apothecary needle and thread (2 diamond marks) - $2
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Soldier's daily wages (5 diamond marks) - $5
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		<span class="_2v4IIjPhKL0PDaWaWtjJ1E _2v4IIjPhKL0PDaWaWtjJ1E _15VS32zBYFUDI5ssldQhEK"><span class="_3mIYu0jAt23sIWGr4pFcI">Bowl of firemoss, each (1 garnet broam for three bowls)- $6.60 per bowl</span></span><br>
		 
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Adolin's tip to Kaladin (1 emerald chip) - $10
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Apothecary larmic mucus (2 ruby marks) - $20
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		<span class="_2v4IIjPhKL0PDaWaWtjJ1E _2v4IIjPhKL0PDaWaWtjJ1E _15VS32zBYFUDI5ssldQhEK"><span class="_3mIYu0jAt23sIWGr4pFcI">Mraize tips Mem for getting the aether from his suit (3 ruby marks) - $30</span></span>
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Apothecary lister's oil (2 sapphire marks) - $50
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Palanaeum alcove rental (2 sapphire marks) - $50
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		<span class="_2v4IIjPhKL0PDaWaWtjJ1E _2v4IIjPhKL0PDaWaWtjJ1E _15VS32zBYFUDI5ssldQhEK"><span class="_3mIYu0jAt23sIWGr4pFcI">Shallan's mistaken offer for candied fruit (1 emerald mark) - $50</span></span>
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Apothecary knobweed sap, per bottle (2 sapphire marks) $50<br>
		 
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		<span class="_2v4IIjPhKL0PDaWaWtjJ1E _2v4IIjPhKL0PDaWaWtjJ1E _15VS32zBYFUDI5ssldQhEK"><span class="_3mIYu0jAt23sIWGr4pFcI">Copy of <em>Words of Radiance</em>, found by Gaz (2 sapphire broams) - $200</span></span>
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		1 emerald broam (largest denomination) - $200
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		<span class="_2v4IIjPhKL0PDaWaWtjJ1E _2v4IIjPhKL0PDaWaWtjJ1E _15VS32zBYFUDI5ssldQhEK"><span class="_3mIYu0jAt23sIWGr4pFcI">Shallan's weekly stipend (3 emerald broams) - $600</span></span>
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Renegotiated price for Shallan's books (2 emerald broams and 3 sapphire broams) - $700<br>
		 
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		<span class="_2v4IIjPhKL0PDaWaWtjJ1E _2v4IIjPhKL0PDaWaWtjJ1E _15VS32zBYFUDI5ssldQhEK"><span class="_3mIYu0jAt23sIWGr4pFcI">Tvlakv's trade wagon and 5 slaves (5 emerald broams) - $1,000</span></span>
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Artmyrn's initial offer for Shallan's books (10 emerald broams) - $2,000
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		<span class="_2v4IIjPhKL0PDaWaWtjJ1E _2v4IIjPhKL0PDaWaWtjJ1E _15VS32zBYFUDI5ssldQhEK"><span class="_3mIYu0jAt23sIWGr4pFcI">Shallan's aluminum necklass (10 emerald broams) - $2,000</span></span>
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		<span class="_2v4IIjPhKL0PDaWaWtjJ1E _2v4IIjPhKL0PDaWaWtjJ1E _15VS32zBYFUDI5ssldQhEK"><span class="_3mIYu0jAt23sIWGr4pFcI">Gaz's debt (80 ruby broams) - $3,200</span></span>
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		<span class="_2v4IIjPhKL0PDaWaWtjJ1E _2v4IIjPhKL0PDaWaWtjJ1E _15VS32zBYFUDI5ssldQhEK"><span class="_3mIYu0jAt23sIWGr4pFcI">Wikim and Balat's knives, each (20 emerald broams) - $4,000</span></span><br>
		 
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Dalanar's offered price to purchase Sadaes's bridgemen, each (60 emerald broams) - $12,000<br>
		 
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Palanaeum chit of admittance (1,000 sapphire broams) - $100,000
	</li>
	<li class="_1qeIAgB0cPwnLhDF9XSiJM">
		Sadaes would reject even if Dalinar this much for bridgemen, each (1,000 emerald broams) - $200,000<br>
		 
	</li>
</ul>

<div data-role="contentPage">
	<hr data-role="contentPageBreak">
</div>

<p class="_1qeIAgB0cPwnLhDF9XSiJM">
	Again, I'm not ecoomist or historian, but I think these sound somewhat reasonable? Could be shifted around a little one way or the other, but I think the order of magnitude feels right.
</p>

<p class="_1qeIAgB0cPwnLhDF9XSiJM">
	There are people (in extreme poverty) in our world who live on $2 per day. The wages for the sailors does seem a bit low, but both they and the bridgemen also essentially have free housing and (presumably) meals. So that's more of a stipend than a wage. Seems like a very reasonable wage for what is essentially a pre-industrial indentured servant?
</p>

<p class="_1qeIAgB0cPwnLhDF9XSiJM">
	The minimum pricepoint of $0.20 STILL seems weirdly high, but I don't think we can go much lower. The bread doesn't seem bad, though it's odd to me candied fruit costs the same. What do you charge for a non-candied piece of fruit? Do people just not do that? They'd buy more than one piece? Perhaps the people at the bottom of society tend to just barter goods directly instead of using spheres.
</p>

<p class="_1qeIAgB0cPwnLhDF9XSiJM">
	Books costing a few hundred dollars apiece seems somewhat reasonable? I expect books cost even more, prior to the printing press. But then Roshar is a bit more culturally developed despite that technology, so demand is probably bringing that price down.
</p>

<p class="_1qeIAgB0cPwnLhDF9XSiJM">
	Dalinar's offer to buy the bridgemen is crazy. There were about 1,000 bridgemen I believe, which puts the total cost (if Sadeas had agreed) at $12 million. Apparently Dalinar could afford that (if only barely) while Sadeas's counter-offer of $200 million was going too far. So that's interesting.
</p>

<div data-role="contentPage">
	<div data-role="contentPage">
		<hr data-role="contentPageBreak">
	</div>

	<p>
		 
	</p>

	<p>
		<strong>EDITS:</strong>
	</p>

	<p>
		<em>2021-08-17</em>
	</p>

	<ol>
		<li>
			I saw someone point out a WoB in which Brandon says that 1 dollar = 1 clearmark "sounds about right". (<a href="https://wob.coppermind.net/events/75/#e4380" ipsnoembed="true" rel="external nofollow">https://wob.coppermind.net/events/75/#e4380</a>) Now, this is the kind of detail that I REALLY don't think Brandon is likely to remember off the top of his head, especially in the middle of a signing. So I don't put much weight in this. But it's <em>something</em> and it's exactly what I had here. So that's nice.
		</li>
		<li>
			Thanks to Caleb Richards on Facebook for catching an error on the cost of the Palanaeum alcove rental. Had $500 when it should have been $50.
		</li>
		<li>
			I did a quick search through Dawnshard and Rhythm of War and didn't find anything of note to add. Didn't get any transactions in the book where the spheres exchanged are made clear. So this should be up-to-date through RoW.
		</li>
	</ol>
</div>
]]></description><guid isPermaLink="false">693</guid><pubDate>Mon, 03 Feb 2020 16:44:00 +0000</pubDate></item><item><title>Stormlight Archive Timeline (v2.3)</title><link>https://www.17thshard.com/blogs/entry/692-stormlight-archive-timeline-v23/</link><description><![CDATA[
<p>
	Updated my Stormlight Archive timeline again this weekend. Not an exciting update, but figured I'd write a post anyways.
</p>

<p>
	The main changes on this version involved reconciling my timeline with (what I understand to be) Karen's timeline from the Oathbringer beta read, which Alice and Lyndsey have been referencing on their <a href="https://www.tor.com/series/oathbringer-reread-brandon-sanderson/" rel="external nofollow">Tor Oathbringer Reread</a>. They're <em>almost</em> through the entire book now, so I had quite a bit to work through. I shifted around a few of my dates to match Karen's where possible... Unfortunately, there are several things that I strongly disagree with, and so I have stuck with my own dates in these cases. At some point I want to write up my issues in a concise way and send it to Karen. Some are relatively meaningless in the grand scheme of things, but others could potentially matter in one way or another, I think. Of course, it's worth mentioning that this is just supposedly the beta timeline--entirely possible the final/official timeline has many things corrected. In any case, my main issues include:
</p>

<ul>
<li>
		I may have mentioned this previously, (I pointed it out to Peter loooong ago) but Shallan's OB Part 1 chapters are off by a couple of days, relative to when the Everstorms and the first highstorm are referenced.
	</li>
	<li>
		Several of Dalinar's flashbacks seem to be a little off. For most it's maybe within reasonable rounding error, but there was at least 1 or 2 that's clearly off by a few years. Maybe a typo?
	</li>
	<li>
		I finally worked through all of the Moash stuff, and I think some of her dates there are a little odd.
	</li>
	<li>
		The biggest and most complicated problem is Oathbringer Part 4... I was concerned that the Shadesmar sequence didn't line up right, and it seems I was entirely correct. There are references clearly linking the Shadesmar group from the day they enter to the day they reach Celebrant. The time spent on Honor's Path is a little vague. And then there are clear references linking the group from Honor's Path to Thaylen City. There's not any <em>contradictions</em>. The problem is that the travel times on the two Shadesmar ships is HIGHLY inconsistent. They spend something like 2 or 3 days traveling from Riino's lighthouse to Celebrant... And then they spend several weeks traveling from Celebrant to... somewhere nearly Thaylenah. The exact locations of the lighthouse and the place where the group abandons ship are not entirely clear. But honestly, if you look at a map and pick a borderline-unreasonable, best case scenario for each... It doesn't make sense at all. Especially considering there's an explicit mention that Honor's Path is significantly faster than Ico's ship. Oh well... Maybe I can convince them to make an edit for the 10th anniversary edition. <img alt=":)" data-emoticon="true" height="20" src="https://uploads.17thshard.com/emoticons/default_smile.png" srcset="https://uploads.17thshard.com/emoticons/smile@2x.png 2x" title=":)" width="20">
</li>
</ul>
<p>
	That's all the negative stuff. I was pleased to find that I was fairly close (or dead on) with most of my dates--particularly for the Part 3 finale. Peter also answered some questions I had about a few minor things, so those are worked out. I've added Kaladin's Oathbringer memories/flashbacks, so with the Moash stuff done that should be everything from OB!
</p>

<p>
	The reread hasn't quite covered the end of the book, and it LOOKS like Karen shifted the Battle of Thaylen City back an extra day from where I have it. But I'm going to say we're good enough for now. Unless there's some major WoB or new revelation, the next stop will probably be a Stormlight 4 update!
</p>
]]></description><guid isPermaLink="false">692</guid><pubDate>Mon, 03 Feb 2020 15:36:03 +0000</pubDate></item><item><title>Why Roshar's Moons Don't Make Sense</title><link>https://www.17thshard.com/blogs/entry/683-why-roshars-moons-dont-make-sense/</link><description><![CDATA[
<p>
	This comes up in conversations occasionally and I've been meaning to write up a concise and simple explanation for a while now. So here we go.
</p>

<p>
	But before I say anything else, I feel like I need to emphasize that I don't want to come across like I'm complaining about the books. Stormlight Archive is my absolute favorite series and this is such an obscure detail. Astronomy and orbital mechanics is a low-key passion for me (I blame Kerbal Space Program, mostly), so when I'm reading a book that I love and see information about this topic I can't help but dig into it. Brandon and his team do a LOT of work to make all of his fantastical worldbuilding make sense. They can't knock it out of the park every time. Maybe they'll look into this when doing the Stormlight leatherbounds and find a way to "fix" it. Maybe they won't--Roshar's moons are really imaginative, so why throw that out over some minor issues that 99% of readers will never even stop to consider? I'm just writing this up because I enjoy exploring the "science" of these books. Sometimes it doesn't work out nicely... and that's okay. It's fun to do the math regardless, and I'm just thankful Brandon put enough into the books that I can overthink it this much. <img alt=":)" data-emoticon="true" height="20" src="https://uploads.17thshard.com/emoticons/default_smile.png" srcset="https://uploads.17thshard.com/emoticons/smile@2x.png 2x" title=":)" width="20"></p>

<p>
	<strong>The Situation</strong>
</p>

<p>
	I want this to be accessible for people who know very little about astronomy, so let's start with some quick basics. Below is a simple image of Roshar from "above". We're looking "down" on the North pole here.You can see which way it rotates relative to the Sun. You can see where the sun is setting and where it's rising. Note that the continent is actually in the <a href="https://www.17thshard.com/blogs/entry/677-globe-of-roshar/" rel="">southern hemisphere</a> (I think it's one of the TWoK maps that shows the equator along the edges in a subtle way). For simplicity, in this post I'm just going to look at points along the equator. Also note that the continent spans about 120 degrees longitude, and Iri/Shinovar are about 90 degrees longitude behind the Shattered Plains. In other words, sunset on the Shattered plains is noon in Shinovar. Midnight in Shinovar is dawn on the Shattered Plains.
</p>

<p>
	<img alt="1.PNG" class="ipsImage ipsImage_thumbnailed" data-fileid="32489" data-unique="oz8kjmpvt" src="https://uploads.17thshard.com/monthly_2019_11/1.PNG.c60b88f7bcb364819632f03bbde434d8.PNG" style=""></p>

<p>
	We know that Roshar's moons orbit the planet once per day (every 20 Rosharan hours) because they rise and set the same time every night. This is something the books are never 100% explicit on, but it's heavily implied and <a href="https://wob.coppermind.net/events/305-miscellaneous-2014/#e8096" rel="external nofollow">has been confirmed</a>. (Technically, they orbit a *bit* faster and precess slightly so that they keep their position relative to the Sun at all times of the year.) This nearly implies a geosynchronous orbit, where a satellite ends up over the same spot on the ground every day. But it can't be that or the moons would be up all day and night. Viewed from the ground they'd just sort of wobble back and forth around a fixed point in the sky. And that's not the case. They rise in the east, set in the west, and are only up for a few hours. (TWoK 2 &amp; 23, among others) This means they are in a retrograde orbit (they go around clockwise) and it means they're in an elliptical orbit with the low point on the nighttime side of Roshar. This is what you need to get such behavior. Here's a very simplified approximation of one such moon:
</p>

<p>
	<img alt="2.PNG" class="ipsImage ipsImage_thumbnailed" data-fileid="32490" data-unique="fg8t2iq8h" src="https://uploads.17thshard.com/monthly_2019_11/2.PNG.42ef79f93a3647b39e69f4131006a144.PNG" style=""></p>

<p>
	There are 3 of them of course. The Arcanum Unbounded star chart of Roshar suggests they are all at slightly different orientations relative to the sun. They are also inclined orbits, which is necessary to have the rise/set in the east/west for a viewer in the southern hemisphere. But for this post we're just going to keep it simple and pretend they're on the same plane as the equator.
</p>

<p>
	The order and timing of the moons as observed from the Shattered Plains is (and I'm using a 20-hour clock)... Salas rises just after sunset, around 15:00. Salas is up for about 2 Rosharan hours. Salas sets and we have an hour of darkness before Nomon rises. ("the hateful hour") Nomon rises around 18:00 and is up for 3-4 hours. Nomon sets as Mishim rises, around 1:00 or 2:00, and Mishim sets at sunrise (5:00).
</p>

<p>
	<strong>So why don't they make sense?</strong>
</p>

<p>
	Let's zero-in on the first moon, Salas. The moon should JUST become visible on the horizon at sunset, so the viewer's line of site looks something like this.
</p>

<p>
	<img alt="3.PNG" class="ipsImage ipsImage_thumbnailed" data-fileid="32491" data-unique="dcdzce0m8" src="https://uploads.17thshard.com/monthly_2019_11/3.PNG.924d88f19e4155709af82080d4a28ea2.PNG" style=""></p>

<p>
	Now we skip ahead 2 hours. Roshar turns about 36 degrees during that time (2 / 20 hours = 10%), so I've put an X at our viewer's new location. At this time, Salas is setting behind the horizon. So their line of sight looks like this. So consider what a person at points Y (2 hours behind the Shattered Plains) and Z (Shinovar) are seeing. It's pretty clear that they can't possibly see the moon rise at sunset. In Shinovar, Salas will be high in the sky already in their afternoon.
</p>

<p>
	<img alt="4.PNG" class="ipsImage ipsImage_thumbnailed" data-fileid="32492" data-unique="ztue0jec7" src="https://uploads.17thshard.com/monthly_2019_11/4.PNG.12b53a393b224db2266341ffe757efcd.PNG" style=""></p>

<p>
	Now, to be fair, the orbital path that I've drawn for Salas is somewhat arbitrary here. But the fundamental problem can't be fixed with a different orbit. If you want to slow the moon down, so that it's simply visible around sunset in Shinovar, that means it's going to be visible longer in the Shattered Plains' night sky.
</p>

<p>
	<img alt="5.PNG" class="ipsImage ipsImage_thumbnailed" data-fileid="32493" data-unique="waua8ldqp" src="https://uploads.17thshard.com/monthly_2019_11/5.PNG.264b2005b3899f52e4657158670d8c33.PNG" style=""></p>

<p>
	<strong>Solutions?</strong>
</p>

<p>
	I can't help but wonder what could be done differently. If you were going to try and "fix" the books, what approach would you take? (Aside from the option of just ignoring the problem and not thinking about it too much)
</p>

<p>
	The simple option is to just make the orbits work for the Shattered Plains and say that they ARE indeed not visible for some of western Roshar. Maybe they are visible during the day. The problem with this is that Szeth seems to suggest they don't do that. The Shin are actually where we get a name ("hateful hour") for the time between Salas and Nomon. But that could be changed. And there are some other timings that would need to be adjusted, but not too many.
</p>

<p>
	Alternatively, you <em>might</em> be able to push all of them back in their orbits a bit so that they all show up in the night sky for everyone across the continent. This would probably result in them moving faster across the sky. And it would probably mean that eastern Roshar has a few hours of darkness between sunset and Salas while western Roshar has a few hours of darkness between Mishim and sunrise.
</p>

<p>
	Another option is to have them move more slowly. It wouldn't be hard to have them set to all rise at roughly the same time, if you turn the orbit the right way. It simply means they're going to be relatively high in the sky for that portion, and that means they're going to be visible for much longer. Their movement would almost be more from Roshar turning than from the moons' own movement. (i.e. more like the way our own moon moves across the sky) This means their visibility will overlap and it means we have to toss out the hateful hour.
</p>

<p>
	Of course, if someone sees something I'm missing, please let me know. <img alt=":)" data-emoticon="true" height="20" src="https://uploads.17thshard.com/emoticons/default_smile.png" srcset="https://uploads.17thshard.com/emoticons/smile@2x.png 2x" title=":)" width="20"> I HAVE simplified this by keeping things on Roshar's equatorial plane, but I'm fairly confident that you get <em>more or less</em> the same thing if we incline the orbits a little and view the moons from a point in the southern hemisphere.
</p>
]]></description><guid isPermaLink="false">683</guid><pubDate>Mon, 25 Nov 2019 17:55:00 +0000</pubDate></item><item><title>Globe of Roshar</title><link>https://www.17thshard.com/blogs/entry/677-globe-of-roshar/</link><description><![CDATA[
<p>
	Finally got around to something I've wanted to do for a long time. <strong><a href="https://www.maptoglobe.com/S1ZUsRkvH" rel="external nofollow">Make a globe of Roshar!</a></strong>
</p>

<p>
	The site doesn't work very well on mobile, so here's some images:
</p>

<p>
	<a class="ipsAttachLink ipsAttachLink_image" data-fileid="31197" href="//uploads.17thshard.com/monthly_2019_09/5d857f6bbf7d6_Screenshot2019-09-20at8_49_57PM.png.44712539fad69b7b73c4d991cac2d0b3.png" rel=""><img alt="Screenshot 2019-09-20 at 8.49.57 PM.png" class="ipsImage ipsImage_thumbnailed" data-fileid="31197" data-unique="xm7nqo2sy" src="https://uploads.17thshard.com/monthly_2019_09/5d857f6de9de9_Screenshot2019-09-20at8_49_57PM.thumb.png.ea25a805d285b28eb3438c0d20254f7b.png" style="width: 500px; height: auto;"></a> <img alt="Screenshot 2019-09-20 at 8.51.39 PM.png" class="ipsImage ipsImage_thumbnailed" data-fileid="31195" data-unique="lxa0g03az" src="https://uploads.17thshard.com/monthly_2019_09/5d857f61845ae_Screenshot2019-09-20at8_51_39PM.png.db02657ab774e1be75e3cf0b46eced01.png" style="width: 366px; height: auto;">
</p>

<p>
	First need to say thanks to u/Stoneward13 on Reddit who created the <a href="https://www.reddit.com/r/Stormlight_Archive/comments/d4kr1c/roshar_reimagined_a_higher_resolution_and_more/" rel="external nofollow">beautiful high-resolution map</a> that I used for this. 
</p>

<p>
	The trick was getting the projection right. <a contenteditable="false" data-ipshover="" data-ipshover-target="https://www.17thshard.com/profile/6699-otto-didact/?do=hovercard" data-mentionid="6699" href="https://www.17thshard.com/profile/6699-otto-didact/" id="ips_uid_3913_21" rel="">@Otto Didact</a> identified the <a href="https://coppermind.net/wiki/Roshar#/media/File:OB_Roshar.jpg" rel="external nofollow">map from Oathbringer</a> as an "azimuthal equidistant" projection while the "Map To Globe" site I used required an equirectangular projection. With a bit of patience I finally discovered a way in QGIS to mark coordinates on a raster image and have that program pump out the <a href="https://i.imgur.com/8yIkVh0.jpg" rel="external nofollow">equirectangular</a> projection!
</p>

<p>
	So here you have it. I've positioned it at the appropriate latitude, with the equator passing through the center of Kadrix island. To anybody not aware, yes, Roshar is mostly ocean. Brandon has stated that there are no other major landmasses. It's possible that ice caps exist, (seems like Yalb mentions tales of a southern ice cap?) but I haven't speculated on that. Maybe I'll circle back around to it. The continent is a bit smaller than Asia. More details on that sort of thing here: 
</p>
<iframe data-embedcontent="" frameborder="0" src="https://www.17thshard.com/blogs/entry/634-roshar-physical-characteristics-and-areas/?do=embed"></iframe>

<p>
	Under the "Options' menu you can toggle longitude/latitude lines. (if comparing with the Oathbringer map, typical lines won't line up right because Roshar uses 200 "degrees" in a circle) And play with some other tweaks, like lighting. 
</p>

<p>
	<s>But my favorite feature is the "Measure distance" button. Click that and enter Roshar's radius (about 5663 km) and it report the distance between two points you select.</s> Unfortunately, last I checked it looks like the measure distance feature is broken. Thankfully such a feature was added to <a href="https://roshar.17thshard.com" rel="external nofollow">roshar.17thshard.com</a> so at least there's that. <img alt=":)" data-emoticon="true" height="20" src="https://uploads.17thshard.com/emoticons/default_smile.png" srcset="https://uploads.17thshard.com/emoticons/smile@2x.png 2x" title=":)" width="20">
</p>

<p>
	Edit: We have since realized that the projection used for this was just a little bit off. An azumithal equidistant projection works by picking a center point--the one that equidistant azumiths are taken from. (It doesn't have to be the center of the map you end up with. You can project the entire globe and then crop out any portion of it that you want.) While working on latitude/longitude lines for roshar.17thshard.com we realized the center point we were using was off. That's the point I used to turn the 2D map back into a globe, so the globe is a little off. Not by a lot, but I wanted to note it here. More details about what the center point should be:
</p>
<iframe data-embedcontent="" frameborder="0" src="https://www.17thshard.com/blogs/entry/821-rosharan-miles-and-other-units-of-distance/?do=embed"></iframe>

<p>
	 
</p>
]]></description><guid isPermaLink="false">677</guid><pubDate>Sat, 21 Sep 2019 03:22:00 +0000</pubDate></item><item><title>Stormlight Archive Timeline (v2.2)</title><link>https://www.17thshard.com/blogs/entry/674-stormlight-archive-timeline-v22/</link><description><![CDATA[
<p>
	Okay, another little Stormlight Timeline update.
</p>

<p>
	The latest version is here: <a href="https://docs.google.com/spreadsheets/d/1zq5bJoKE83ggDCjH43i1hZi0CIpB2iAx7v37zQPVFK0" ipsnoembed="true" rel="external nofollow">https://docs.google.com/spreadsheets/d/1zq5bJoKE83ggDCjH43i1hZi0CIpB2iAx7v37zQPVFK0</a>
</p>

<div class="_3cjCphgls6DH-irkVaA0GM" data-test-id="comment">
	<div class="_292iotee39Lmt0MkQZ2hPV RichTextJSON-root" style="color:#1A1A1B" theme="[object Object]">
		<p class="_1qeIAgB0cPwnLhDF9XSiJM">
			<strong>Additions</strong>
		</p>

		<p class="_1qeIAgB0cPwnLhDF9XSiJM">
			I finally took the time to actually <em class="_7s4syPYtk5hfUIjySXcRE">finish</em> the timeline. Most of the Urithiru plot in Part 4 still wasn't in there. Some of Dalinar's flashbacks which were tied to Part 4 dates (including the Nightwatcher visit), weren't in there. Moash and Szeth weren't in there. And most of the interludes weren't in there. That has been remedied!
		</p>

		<p class="_1qeIAgB0cPwnLhDF9XSiJM">
			There are two (or three?) Kaladin flashbacks that I haven't attempted to place yet, though these would be heavy speculation. Otherwise, that's pretty much everything I can think of that ought to be in it. If anyone ever sees something that seems missing please let me know!
		</p>

		<p class="_1qeIAgB0cPwnLhDF9XSiJM">
			<strong>Reconciliation Effort</strong>
		</p>

		<p class="_1qeIAgB0cPwnLhDF9XSiJM">
			The folks doing Tor's Oathbringer reread have access to a preliminary timeline produced by Brandon's team, and they've been sharing the dates they have for each chapter in their weekly reread posts. So I finally took some time to reconcile my timeline with those dates. For the most part this just involved shifting things around within the bounds of the assumptions I originally made. Tricky because of how many strings there are tying events together, but it all worked out. LOTS of Oathbringer events got shifted one way or the other, though very few of them were affected in a significant way. The vast majority were a matter of some thing shifting a few days sooner or later. In any case, my timeline MOSTLY matches theirs now. (and thus, hopefully, the official timeline) When Tor gets to the end of the book, I'll make sure to reconcile what I have for the remainder of the book!
		</p>

		<p class="_1qeIAgB0cPwnLhDF9XSiJM">
			<strong>Timeline Issues</strong>
		</p>

		<p class="_1qeIAgB0cPwnLhDF9XSiJM">
			There are a FEW things that appear to be errors, so I've stuck with my own guesses in those cases. This was another big goal of doing this. I've <em>known</em> that there are some issues with the timeline Tor is using. Going through one chapter at a time and comparing their date with my own (and my basis) allowed me to pinpoint exactly where issues were found. Notable issues that need a closer look include:
		</p>

		<ul>
<li class="_1qeIAgB0cPwnLhDF9XSiJM">
				Some of Dalinar's flashbacks seem to list the wrong year
			</li>
			<li class="_1qeIAgB0cPwnLhDF9XSiJM">
				Jasnah's birthday is off. TWoK stated that she was 34 years old, but that doesn't match up with where Dalinar's flashbacks place her birth. I'm guessing TWoK may need to be retconned to make her a year younger. That's a simple fix compared to reworking some of the flashback continuity.
			</li>
			<li class="_1qeIAgB0cPwnLhDF9XSiJM">
				Some of Shallan's activity in Oathbringer Part 1 appears to be off. But this is just official dates in the background. I don't think the book would actually be affected.
			</li>
			<li class="_1qeIAgB0cPwnLhDF9XSiJM">
				I think there's a few issues with the dates for Moash. Again, nothing that would affect the book.
			</li>
			<li class="_1qeIAgB0cPwnLhDF9XSiJM">
				The Shadesmar sequence doesn't match up to me. The description of how much time passes from their entrance to their exit is a bit shorter, in my opinion, than what the timeline requires. I think Brandon may need to massage some of the descriptions of how much time is passing.
			</li>
			<li class="_1qeIAgB0cPwnLhDF9XSiJM">
				Some of the Everstorms seem to hit quite a bit off from where they SHOULD. This mostly doesn't bother me. The book states that they vary a bit. But the timing of the last one in Kholinar looks strange to me.
			</li>
			<li class="_1qeIAgB0cPwnLhDF9XSiJM">
				Szeth and the Skybreakers spent FOUR days flying from Purelake to Marat. They make several stops, but it still seems a little weird compared to other flight times that we have.
			</li>
		</ul>
</div>
</div>

<p>
	 
</p>
]]></description><guid isPermaLink="false">674</guid><pubDate>Wed, 28 Aug 2019 22:42:11 +0000</pubDate></item><item><title>Stormlight Archive Timeline (v2.1)</title><link>https://www.17thshard.com/blogs/entry/664-stormlight-archive-timeline-v21/</link><description><![CDATA[
<p>
	I've been itching to do a quick update post on my Stormlight Archive Timeline as I've hit a big milestone. In my last post on the timeline I mentioned wanting to convert from a spreadsheet to a database. And I've done it!
</p>

<p>
	Link to the newest version: <a href="https://docs.google.com/spreadsheets/d/1zq5bJoKE83ggDCjH43i1hZi0CIpB2iAx7v37zQPVFK0" ipsnoembed="true" rel="external nofollow">https://docs.google.com/spreadsheets/d/1zq5bJoKE83ggDCjH43i1hZi0CIpB2iAx7v37zQPVFK0</a>
</p>

<p>
	<span style="font-size:18px;">Back End Changes</span>
</p>

<p>
	Previously, every entry in the timeline utilized a single row in the spreadsheet. This put some restrictions on how the date was calculated and it meant my list of sources were jammed together. In my database I've broken everything down into three tables. An "event" is simply some event that occurs (along with a category for sorting and any book chapters that the event occurs in). Next is a table of "intervals" which define the number of days (and any range of error) between two events. Lastly is a table of "sources" which link any relevant sources and my notes to each interval.
</p>

<p>
	Now I can make a date dependent on multiple intervals (it uses the average, more or less). This is very useful for something like Gavilar's assassination, where we several potential date ranges based on different sources. The database is able to find the average date and the overlapping error range so that we get something as specific as possible. I can also create a new record for every source I use, which makes them a lot easier to organize and sort through. One downside is that I simply have a local copy of the database, and updating is a manual process. If I make changes, I have to export new spreadsheets and paste them in on top of the old copies. This isn't as bad as it sounds though, because I wanted to separate the presentation from the calculations regardless. The final product now is mostly just text, which means the Google Sheet loads up and operates a lot faster. Conditional formatting slows it down, but that was going to be there regardless. (And I can always spit out an unformatted version for maximum speed.) It also means you can use Ctrl+F to atually search the document, which is super helpful!
</p>

<p>
	<span style="font-size:18px;">Front End Changes</span>
</p>

<p>
	In this latest version I've added a few more events than I had previously, and made a few corrections. All small stuff for the most part. The most notable additions are some Pre-History events which are very speculative. But we DID get some more details on the Desolations via WoB, and after some good conversation in the "History of Roshar" Shardcasts, I felt like there was enough information for it not to look stupid. <img alt=":)" data-emoticon="true" height="20" src="https://uploads.17thshard.com/emoticons/default_smile.png" srcset="https://uploads.17thshard.com/emoticons/smile@2x.png 2x" title=":)" width="20"></p>

<p>
	I've also added a few "filter" options. Under the "Spoiler Filter" sheet you can check/uncheck boxes to control which event categories are displayed. Theoretically this can be used to hide spoilers, though obviously you can use that however you want. More interesting is a filter (in the top right corner) which allows users to filter out events that are below different levels of "confidence". The color of event ID numbers gives a hint at how confident I am in their date. Something marked 1 is absolutely known with explicit support while something marked 5 was pulled out of thin air for the sake of putting something on the timeline. You can now use this little dropdown to hide events below a confidence threshhold.
</p>

<p>
	One other change is that the event numbers act as hyperlinks to cells on other sheets. If you click the event ID number for something on the timeline, it will pop you over onto that event's row(s) on the References sheet. So you can instantly jump over and see what sources were used to nail down each event.
</p>

<p>
	Lastly, there's an Ages sheet, which lists the age of each character (with a known age) next to each event. The Ages column on the Timeline sheet references these numbers, though it can also be used if you want to directly compare characters side by side.
</p>

<p>
	<span style="font-size:18px;">Future Plans</span>
</p>

<p>
	I've still got some Oathbringer events missing, so the next notable update will happen whenever I can finish those off. Many of those that are missing simply didn't have enough information (that I could find) to place the event. The good news is that Tor's Oathbringer reread posts have been listing dates for each chapter based on the gamma read timeline. I'm not assuming these are canonical, but they make for a great basis in lieu of something more specific. So I'm currently working through these, trying to reconcile our timelines.
</p>

<p>
	The bad news is that the Tor Reread only moves at 1 or 2 chapters per week, and they're only about 2/3 through the book! Also, I don't agree with every date provided. There are occaisional small discrepancies that I think will need to be adjusted on Karen's end (and other cases where mine need adjusting, but that's easy to fix...). In and of itself this isn't a big deal. The problem is that I don't know how the gamma timeline is CONNECTED, so if one date is wrong I have no way of knowing how a change there will impact subsequent dates.
</p>

<p>
	So it's going to be a while before (1) Tor's Reread reaches the end of the book and (2) I am able to finish filling in my timeline with that information. Most of the holes in my timeline are from Part 4, so I'm looking forward to that. I very well may update my timeline periodically, if I feel like I've added/changed anything significant. I will update the version number in the spreadsheet's title when I do this. But I likely won't mention those updates here or in the forums as it will just be dates added/changed. When I AM totally caught up I will probably update my timeline post in the forums. I'll also probably make another blog post that covers any discrepancies I think I've found, either with the gamma timeline or with contradictions in the book itself.
</p>
]]></description><guid isPermaLink="false">664</guid><pubDate>Wed, 03 Apr 2019 20:35:27 +0000</pubDate></item><item><title>Stormlight Archive Timeline</title><link>https://www.17thshard.com/blogs/entry/658-stormlight-archive-timeline/</link><description><![CDATA[
<p>
	Since this has been primarily a personal project, I figure it deserved a post in this blog as well. I'm not going to talk about the content of the timeline itself here. This is more about the background and (ongoing) development of it.
</p>

<p>
	Link to the timeline for reference: <a href="https://docs.google.com/spreadsheets/d/1Wdigy6ZNX4EGRAaUskfM0LXNANksyM1JintSn4yKSyM/edit#gid=2005334307" ipsnoembed="true" rel="external nofollow">https://docs.google.com/spreadsheets/d/1Wdigy6ZNX4EGRAaUskfM0LXNANksyM1JintSn4yKSyM/edit#gid=2005334307</a>
</p>

<p>
	<strong>Inspiration</strong>
</p>

<p>
	There were two primary inspirations for creating this timeline.
</p>

<p>
	First was <a href="http://www.stevenac.net/wot/wotchron.htm" rel="external nofollow">this Wheel of Time timeline</a>, which mostly just made me jealous that we didn't have a similar overall timeline in the works.
</p>

<p>
	Second was the <a href="https://coppermind.net/wiki/Words_of_Radiance/Timeline" rel="external nofollow">Words of Radiance Timeline</a> that was primarily created by WeiryWriter. Between the Everstorm countdown and a list of highstorm dates revealed in an epigraph, were were able to pin down most of the events in Words of Radiance with great accuracy. Weiry had started a timeline for The Way of Kings, but there just wasn't much concrete information to work with in that book, unfortunately. Because these timelines were living on Coppermind, we didn't want to post anything there that was more assumption than fact.
</p>

<p>
	<strong>Concept</strong>
</p>

<p>
	So the idea here is to have a timeline that DOES allow for assumptions and guesswork. But it was important to me that the whole thing be as well-researched and supported as possible. I wanted to support every date on the timeline with some kind of sourced information. Assumptions needed to provide the supporting evidence. And the confidence or certainty in an event needed to be transparent.
</p>

<p>
	I began by importing the Words of Radiance timeline and building out my concept for how this would work. There are two ideas that stood out: "events" and "intervals". An "event" is some event that happens in-world. A point in time that happens on a specific date. An "interval" is some period of time that passes in between events.
</p>

<p>
	Both events and intervals can have a "range" or "error" associated with them. This is introduced by uncertainty and assumptions. For example, if a flashback happened "Five Years Ago", we can use an interval of exactly 5 years... But we know that this doesn't mean <em>precisely 5 years</em>. Brandon isn't being that specific. So we attach some wiggle room to the interval. Instead of an interval of "minus 5 years" we use "minus 5 years, plus or minus 2.5 months". This error introduced by interval uncertainty factors into the dates themselves, of course. And it adds up. So if there was some event that happened "one year plus or minus 2 months" after the flashback of that last example, this event now has +/- 4.5 months of error with respect to the event that the flashback date is based on.
</p>

<p>
	The range alone doesn't account for what I call "confidence". There's a <em>bit</em> of gut feel involved here, and it's certainly true that more error/range tends to come with less confidence. But there are certainly cases where something with a range is still something we can be fairly confident in.
</p>

<p>
	<strong>Development</strong>
</p>

<p>
	After importing Words of Radiance I began to work on The Way of Kings, which is where things got really challenging. You have to really dig into that book, digging for any scrap you can get. For example, at some point there is an implication that Sadeas's bridge crews are supplemented with new men on chachel, the third day of the week. We can use this tidbit later in the book to pin down the days that Lopen and Shen join Bridge Four. Another thing I had to do a lot was work backwards. Most of Kaladin's TWoK timeline is actually worked backwards from the end of the book. Because the time that passes during Part 1 is incredibly ambiguous.
</p>

<p>
	There's also some contradictions, or just things that don't seem to fit very well. A comment by Elhokar at the first feast put the Chasmfiend hunt disaster on a date that doesn't work with the story, for example. Another thing involving the Chasmfiend hunt--Kaladin was strung up for the highstorm on that same day, which doesn't entirely make sense because Sadeas was out on the hunt. Prior to the release of Oathbringer, Karen Ahlstrom gave us some tidbits that helped pin down some of the dates. This helped a lot. Some of them I wasn't entirely sure about, and I regret that I didn't keep better record of those disagreements. In any case, I've tried my best to align my timeline with hers and make note of any clear contradictions that exist.
</p>

<p>
	I got some help pulling together notes for chronology in Oathbringer. It isn't, unfortunately, as precise as WoR was, but Brandon is more free with mentioning the passage of time at least, and Karen seems to be doing a pretty good job of tweaking the numbers so that it makes sense. I have <em>not</em> worked out all of my timeline to match her dates yet, however, because there are a few tweaks here or there that I think need to be made. In any case, I've still got a bit more content from Oathbringer that needs to be worked out.
</p>

<p>
	<strong>Issues</strong>
</p>

<p>
	One frustrating thing about the timeline is that it's SLOW. It takes forever to open/load, and this is only going to get worse with more books. The calculations that happen in the spreadsheet aren't <em>terrible</em>, but every row of the sheet does have more calculations going on than you might think. And on the timeline sheet there's a lot of string concatenations that slow things down pretty badly.
</p>

<p>
	I'm also frustrated by the way each entry has to exist on a single row. There are some cases where an event is based on TWO other events/intervals, and the only way to do this is by doing the math manually. This gets dangerous because many thing in the timeline are subject to change, so a shift in one of those dependencies can cause an error and I wouldn't know it readily. The sources and notes are also crammed into a single cell, which is terribly sloppy organization.
</p>

<p>
	Adding new rows has also caused some problems. Each entry has to be referenced by an ID, and I'm uncomfortable creating these manually for fear of making a mistake.
</p>

<p>
	<strong>Future Plans</strong>
</p>

<p>
	To solve a lot of these problems, I've been looking at moving the whole thing to an offline relational database. Anytime I made a change I would have to manually update the spreadsheet posted online, but I think it should be easy enough to automate most of that process.
</p>

<p>
	The idea is to have 3 separate tables for "events", "intervals", and "sources". Each one has a unique ID. Events are linked to one or more interval--it uses the average resultant date if so, and the overlap of their ranges to determine error. Intervals are linked to one or more sources. I don't have to put events/intervals/sources in some logical row on a spreadsheet. I can just add new ones to the end, letting the database assign them a unique ID. I should be able to build an interface for inputting this info so that I don't have to add it directly to a table myself.
</p>

<p>
	From there it's a simple query to compile everything. And with all of the information in a database I should be able to do a lot of other cool stuff that would be harder to do in the original spreadsheet. For example, I'd like to see what happens if I filter out everything below some confidence threshold. Because the information is more transparent, and not put together by a chain of concatenations, I can do some other cool stuff like create links between an entry on the timeline and the source info.
</p>

<p>
	Here's an output from the (very much work in progress) new version I'm working on: <a href="https://docs.google.com/spreadsheets/d/1zq5bJoKE83ggDCjH43i1hZi0CIpB2iAx7v37zQPVFK0/edit#gid=856252766" ipsnoembed="true" rel="external nofollow">https://docs.google.com/spreadsheets/d/1zq5bJoKE83ggDCjH43i1hZi0CIpB2iAx7v37zQPVFK0/edit#gid=856252766</a>
</p>

<p>
	All this to say, not much should change to the front end of the timeline. But there might be a bit more transparency/functionality, and inputting new data should be a cleaner process.
</p>

<p>
	Anything else to say? I don't think so. Feel free to ask questions though.
</p>
]]></description><guid isPermaLink="false">658</guid><pubDate>Tue, 20 Nov 2018 16:20:07 +0000</pubDate></item><item><title>Stormlight Archive Statistical Analysis</title><link>https://www.17thshard.com/blogs/entry/640-stormlight-archive-statistical-analysis/</link><description><![CDATA[
<p>
	Put together this spreadsheet based on the Statistical Analysis data on <a href="https://coppermind.net/wiki/The_Stormlight_Archive/Statistical_analysis" rel="external nofollow">Coppermind</a>: <a class="ipsAttachLink" data-fileid="23023" href="https://www.17thshard.com/applications/core/interface/file/attachment.php?id=23023" rel="">Stormlight Analysis (2018-9-7).xlsx</a>. The Oathbringer data I entered myself when the book was released, so I feel pretty confident in that. Not certain about the other two, but I expect they're fairly accurate. Had to enter in the Edgedancer data for this myself, along with character genders. Otherwise it was just minor edits, separating the data, etc.
</p>

<p>
	Some fun charts I put together with it below. Let me know if you'd like to see any other interesting comparisons and don't feel like doing it yourself. <img alt=":)" data-emoticon="true" height="20" src="https://uploads.17thshard.com/emoticons/default_smile.png" srcset="https://uploads.17thshard.com/emoticons/smile@2x.png 2x" title=":)" width="20"></p>

<p>
	<strong>Spoilers: </strong>There aren't any real spoilers below, UNLESS you don't want to know which characters appear in future books or how much screen time they get. If you don't want to know that, you've been warned.
</p>

<p>
	<img alt="AFE5l7EVXsj4AAAAAElFTkSuQmCC" 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" 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<p>
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" 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" style="width: 700px; height: auto;"></p>

<p>
	(as someone pointed out on Discord, I've lumped femalen listeners in with female. might be some other odd cases that I overlooked.)
</p>

<p>
	<img alt="UaX331VQ8AACC7r7766v8BZw+nDDTD8FgAAAAASU" 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" 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"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" style="width: 700px; height: auto;"></p>
]]></description><guid isPermaLink="false">640</guid><pubDate>Fri, 07 Sep 2018 16:11:00 +0000</pubDate></item><item><title>Roshar Distances</title><link>https://www.17thshard.com/blogs/entry/635-roshar-distances/</link><description><![CDATA[
<p>
	Distances between several locations on Roshar, in miles.
</p>

<p>
	Full sheet: <a href="https://docs.google.com/spreadsheets/d/19ZZPDVrgVN3eKb6q9epCvTkRWSonkXN8CH69dToWcfM/edit#gid=0" ipsnoembed="true" rel="external nofollow">https://docs.google.com/spreadsheets/d/19ZZPDVrgVN3eKb6q9epCvTkRWSonkXN8CH69dToWcfM/edit#gid=0</a>
</p>

<p>
	(really just go there, it's much better)
</p>

<p>
	<style type="text/css">
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<tbody>
<tr>
<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td data-sheets-value='{"1":2,"2":"location B"}'>
				location B
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"Rall Elorim"}'>
				Rall Elorim
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"Kasitor"}'>
				Kasitor
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"NW Shinovar coastal mountains"}'>
				NW Shinovar coastal mountains
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"W Shinovar coastal mountains"}'>
				W Shinovar coastal mountains
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"SW Shinovar coastal mountains"}'>
				SW Shinovar coastal mountains
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"W Steen"}'>
				W Steen
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"W Tukar"}'>
				W Tukar
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"S Frostlands"}'>
				S Frostlands
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"Shallow Crypts"}'>
				Shallow Crypts
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"New Natanan"}'>
				New Natanan
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value="{&quot;1&quot;:2,&quot;2&quot;:&quot;Dawn's Shadow&quot;}">
				Dawn's Shadow
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"NE tip east coast peninsula"}'>
				NE tip east coast peninsula
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"NE Herdaz"}'>
				NE Herdaz
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"SE Aimia"}'>
				SE Aimia
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"Shinovar coast"}'>
				Shinovar coast
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"Dumadari"}'>
				Dumadari
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"E Akak"}'>
				E Akak
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"Hearthstone"}'>
				Hearthstone
			</td>
			<td data-sheets-formula="=Index(C1:C1,column())" data-sheets-value='{"1":2,"2":"Shattered Plains"}'>
				Shattered Plains
			</td>
		</tr>
<tr>
<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td data-sheets-value='{"1":2,"2":"lat"}'>
				lat
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-3}'>
				-3
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-4}'>
				-4
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-10}'>
				-10
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-16}'>
				-16
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-19}'>
				-19
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-23}'>
				-23
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-29}'>
				-29
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-23}'>
				-23
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-16}'>
				-16
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-14}'>
				-14
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-5}'>
				-5
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-2}'>
				-2
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-14}'>
				-14
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-14}'>
				-14
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-21}'>
				-21
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-3}'>
				-3
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-8}'>
				-8
			</td>
			<td data-sheets-formula="=Index(C2:C2,column())" data-sheets-value='{"1":3,"3":-19}'>
				-19
			</td>
		</tr>
<tr>
<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td data-sheets-value='{"1":2,"2":"long"}'>
				long
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":-14}'>
				-14
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":-18}'>
				-18
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":-24}'>
				-24
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":-28}'>
				-28
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":-27}'>
				-27
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":-29}'>
				-29
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":-26}'>
				-26
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":26}'>
				26
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":35}'>
				35
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":37}'>
				37
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":33}'>
				33
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":34}'>
				34
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":22}'>
				22
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":-28}'>
				-28
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":-31}'>
				-31
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":15}'>
				15
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":25}'>
				25
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":21}'>
				21
			</td>
			<td data-sheets-formula="=Index(C3:C3,column())" data-sheets-value='{"1":3,"3":31}'>
				31
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"location A"}'>
				location A
			</td>
			<td data-sheets-value='{"1":2,"2":"lat"}'>
				lat
			</td>
			<td data-sheets-value='{"1":2,"2":"long"}'>
				long
			</td>
			<td data-sheets-value='{"1":2,"2":"distance"}'>
				distance
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
			<td>
				 
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"Rall Elorim"}'>
				Rall Elorim
			</td>
			<td data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-value='{"1":3,"3":-14}'>
				-14
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":551.7035642509209}'>
				552
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1186.8125614311245}'>
				1187
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1878.9581640798444}'>
				1879
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2237.3579463995343}'>
				2237
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2609.5280234010697}'>
				2610
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2808.899546459298}'>
				2809
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4852.383922539998}'>
				4852
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5439.438508999547}'>
				5439
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5619.059503665768}'>
				5619
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5222.557245269174}'>
				5223
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5304.110895182952}'>
				5304
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3979.304574563892}'>
				3979
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2150.248640572143}'>
				2150
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2383.6054400049493}'>
				2384
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3744.959942275762}'>
				3745
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4312.993189251954}'>
				4313
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3921.6464770336092}'>
				3922
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5066.1392375767955}'>
				5066
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"Kasitor"}'>
				Kasitor
			</td>
			<td data-sheets-value='{"1":3,"3":-3}'>
				-3
			</td>
			<td data-sheets-value='{"1":3,"3":-18}'>
				-18
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":551.7035642509209}'>
				552
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":667.8277645576559}'>
				668
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1327.2667280289807}'>
				1327
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1716.7947804141218}'>
				1717
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2095.0439304230704}'>
				2095
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2345.613713197531}'>
				2346
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4854.893275341458}'>
				4855
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5550.556810846342}'>
				5551
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5843.132320038781}'>
				5843
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5480.884756176306}'>
				5481
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5687.644672614561}'>
				5688
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4403.283830044167}'>
				4403
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1611.3070026126345}'>
				1611
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1835.3539613696876}'>
				1835
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3849.2974550291287}'>
				3849
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4724.195759169973}'>
				4724
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4265.0415189585765}'>
				4265
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5245.101615518784}'>
				5245
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"NW Shinovar coastal mountains"}'>
				NW Shinovar coastal mountains
			</td>
			<td data-sheets-value='{"1":3,"3":-4}'>
				-4
			</td>
			<td data-sheets-value='{"1":3,"3":-24}'>
				-24
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1186.8125614311245}'>
				1187
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":667.8277645576559}'>
				668
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":790.1739815777322}'>
				790
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1361.720240659232}'>
				1362
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1733.2828924904816}'>
				1733
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2107.6332926414734}'>
				2108
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5173.548874152411}'>
				5174
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5961.958448306391}'>
				5962
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6353.0525910181}'>
				6353
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6024.824192441674}'>
				6025
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6316.8163886963885}'>
				6317
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5056.971378025114}'>
				5057
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1182.3379794595003}'>
				1182
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1328.5835630811396}'>
				1329
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4293.8248050778775}'>
				4294
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5371.696462885674}'>
				5372
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4880.663808707965}'>
				4881
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5726.001845839667}'>
				5726
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"W Shinovar coastal mountains"}'>
				W Shinovar coastal mountains
			</td>
			<td data-sheets-value='{"1":3,"3":-10}'>
				-10
			</td>
			<td data-sheets-value='{"1":3,"3":-28}'>
				-28
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1878.9581640798444}'>
				1879
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1327.2667280289807}'>
				1327
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":790.1739815777322}'>
				790
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":670.3451875140485}'>
				670
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":998.8895512461743}'>
				999
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1448.203289894564}'>
				1448
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4917.739023070977}'>
				4918
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5800.187315504077}'>
				5800
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6336.33952820349}'>
				6336
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6086.934867190042}'>
				6087
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6584.082262737581}'>
				6584
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5454.060500550389}'>
				5454
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":441.782320008762}'>
				442
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":538.4095988912787}'>
				538
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4252.701305710908}'>
				4253
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5733.4259613913555}'>
				5733
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5149.687511046263}'>
				5150
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5683.212879171529}'>
				5683
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"SW Shinovar coastal mountains"}'>
				SW Shinovar coastal mountains
			</td>
			<td data-sheets-value='{"1":3,"3":-16}'>
				-16
			</td>
			<td data-sheets-value='{"1":3,"3":-27}'>
				-27
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2237.3579463995343}'>
				2237
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1716.7947804141218}'>
				1717
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1361.720240659232}'>
				1362
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":670.3451875140485}'>
				670
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":381.047492157996}'>
				381
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":778.3290310013025}'>
				778
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4339.544478242595}'>
				4340
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5252.681511205}'>
				5253
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5856.323282036916}'>
				5856
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5662.590786987986}'>
				5663
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6294.236743859735}'>
				6294
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5319.243698816718}'>
				5319
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":241.8080928159956}'>
				242
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":451.2265717183265}'>
				451
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3812.2108975954025}'>
				3812
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5555.475571592887}'>
				5555
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4910.6408725525}'>
				4911
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5203.536526974893}'>
				5204
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"W Steen"}'>
				W Steen
			</td>
			<td data-sheets-value='{"1":3,"3":-19}'>
				-19
			</td>
			<td data-sheets-value='{"1":3,"3":-29}'>
				-29
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2609.5280234010697}'>
				2610
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2095.0439304230704}'>
				2095
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1733.2828924904816}'>
				1733
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":998.8895512461743}'>
				999
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":381.047492157996}'>
				381
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":513.2663971169751}'>
				513
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4209.370269945052}'>
				4209
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5143.41620298564}'>
				5143
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5798.1065479037015}'>
				5798
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5649.458752672315}'>
				5649
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6361.669187198521}'>
				6362
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5489.353091657159}'>
				5489
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":560.4657347517474}'>
				560
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":584.4811036801267}'>
				584
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3814.218735933745}'>
				3814
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5699.201709309928}'>
				5699
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5029.239279167557}'>
				5029
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5154.047912665552}'>
				5154
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"W Tukar"}'>
				W Tukar
			</td>
			<td data-sheets-value='{"1":3,"3":-23}'>
				-23
			</td>
			<td data-sheets-value='{"1":3,"3":-26}'>
				-26
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2808.899546459298}'>
				2809
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2345.613713197531}'>
				2346
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2107.6332926414734}'>
				2108
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1448.203289894564}'>
				1448
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":778.3290310013025}'>
				778
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":513.2663971169751}'>
				513
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3707.1576945631273}'>
				3707
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4645.801270469553}'>
				4646
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5319.90380197372}'>
				5320
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5197.624507165448}'>
				5198
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5964.621417383081}'>
				5965
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5210.63197992651}'>
				5211
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1010.7497546278173}'>
				1011
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1094.3886680996939}'>
				1094
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3387.13354622867}'>
				3387
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5385.917348448718}'>
				5386
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4696.141964939922}'>
				4696
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4683.3381975854645}'>
				4683
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"S Frostlands"}'>
				S Frostlands
			</td>
			<td data-sheets-value='{"1":3,"3":-29}'>
				-29
			</td>
			<td data-sheets-value='{"1":3,"3":26}'>
				26
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4852.383922539998}'>
				4852
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4854.893275341458}'>
				4855
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5173.548874152411}'>
				5174
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4917.739023070977}'>
				4918
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4339.544478242595}'>
				4340
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4209.370269945052}'>
				4209
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3707.1576945631273}'>
				3707
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":945.7578498956274}'>
				946
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1695.0278153902348}'>
				1695
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1757.2972715425844}'>
				1757
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2746.9745501175585}'>
				2747
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3004.573310682517}'>
				3005
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4572.363150528281}'>
				4572
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4758.841390519176}'>
				4759
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1224.5019760935847}'>
				1225
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2873.0368653340424}'>
				2873
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2360.9637145309625}'>
				2361
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1173.383416491995}'>
				1173
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"Shallow Crypts"}'>
				Shallow Crypts
			</td>
			<td data-sheets-value='{"1":3,"3":-23}'>
				-23
			</td>
			<td data-sheets-value='{"1":3,"3":35}'>
				35
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5439.438508999547}'>
				5439
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5550.556810846342}'>
				5551
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5961.958448306391}'>
				5962
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5800.187315504077}'>
				5800
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5252.681511205}'>
				5253
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5143.41620298564}'>
				5143
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4645.801270469553}'>
				4646
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":945.7578498956274}'>
				946
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":793.7521050312029}'>
				794
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1010.7497546278173}'>
				1011
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1990.417728761106}'>
				1990
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2652.670774981641}'>
				2653
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5480.019272195351}'>
				5480
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5681.95349702581}'>
				5682
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1703.890028038013}'>
				1704
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2419.0077949282904}'>
				2419
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2130.90437080479}'>
				2131
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":562.5970872363864}'>
				563
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"New Natanan"}'>
				New Natanan
			</td>
			<td data-sheets-value='{"1":3,"3":-16}'>
				-16
			</td>
			<td data-sheets-value='{"1":3,"3":37}'>
				37
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5619.059503665768}'>
				5619
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5843.132320038781}'>
				5843
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6353.0525910181}'>
				6353
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6336.33952820349}'>
				6336
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5856.323282036916}'>
				5856
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5798.1065479037015}'>
				5798
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5319.90380197372}'>
				5320
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1695.0278153902348}'>
				1695
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":793.7521050312029}'>
				794
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":451.2265717183265}'>
				451
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1254.159262038274}'>
				1254
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2205.9982414626793}'>
				2206
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6068.871578453591}'>
				6069
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6301.149528597836}'>
				6301
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2087.7656197783763}'>
				2088
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1906.7337564775014}'>
				1907
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1857.7752491486553}'>
				1858
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":654.4251195379118}'>
				654
			</td>
		</tr>
<tr>
<td data-sheets-value="{&quot;1&quot;:2,&quot;2&quot;:&quot;Dawn's Shadow&quot;}">
				Dawn's Shadow
			</td>
			<td data-sheets-value='{"1":3,"3":-14}'>
				-14
			</td>
			<td data-sheets-value='{"1":3,"3":33}'>
				33
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5222.557245269174}'>
				5223
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5480.884756176306}'>
				5481
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6024.824192441674}'>
				6025
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6086.934867190042}'>
				6087
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5662.590786987986}'>
				5663
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5649.458752672315}'>
				5649
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5197.624507165448}'>
				5198
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1757.2972715425844}'>
				1757
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1010.7497546278173}'>
				1011
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":451.2265717183265}'>
				451
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":999.552024671876}'>
				1000
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1766.5258159013156}'>
				1767
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5860.440467324999}'>
				5860
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6113.225675816576}'>
				6113
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1850.6282606268758}'>
				1851
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1480.9294091021513}'>
				1481
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1409.10170616955}'>
				1409
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":584.481103680127}'>
				584
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"NE tip east coast peninsula"}'>
				NE tip east coast peninsula
			</td>
			<td data-sheets-value='{"1":3,"3":-5}'>
				-5
			</td>
			<td data-sheets-value='{"1":3,"3":34}'>
				34
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5304.110895182952}'>
				5304
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5687.644672614561}'>
				5688
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6316.8163886963885}'>
				6317
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6584.082262737581}'>
				6584
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6294.236743859735}'>
				6294
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6361.669187198521}'>
				6362
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5964.621417383081}'>
				5965
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2746.9745501175585}'>
				2747
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1990.417728761106}'>
				1990
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1254.159262038274}'>
				1254
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":999.552024671876}'>
				1000
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1357.7889407954174}'>
				1358
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6455.631652110662}'>
				6456
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6738.604052444343}'>
				6739
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2586.4495882771007}'>
				2586
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1010.3910426379607}'>
				1010
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1443.504251756781}'>
				1444
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1575.9069595188241}'>
				1576
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"NE Herdaz"}'>
				NE Herdaz
			</td>
			<td data-sheets-value='{"1":3,"3":-2}'>
				-2
			</td>
			<td data-sheets-value='{"1":3,"3":22}'>
				22
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3979.304574563892}'>
				3979
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4403.283830044167}'>
				4403
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5056.971378025114}'>
				5057
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5454.060500550389}'>
				5454
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5319.243698816718}'>
				5319
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5489.353091657159}'>
				5489
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5210.63197992651}'>
				5211
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3004.573310682517}'>
				3005
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2652.670774981641}'>
				2653
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2205.9982414626793}'>
				2206
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1766.5258159013156}'>
				1767
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1357.7889407954174}'>
				1358
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5428.278789152926}'>
				5428
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5727.174053405646}'>
				5727
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2214.458183738257}'>
				2214
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":348.276915516745}'>
				348
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":671.5637845967167}'>
				672
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2092.918435320211}'>
				2093
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"SE Aimia"}'>
				SE Aimia
			</td>
			<td data-sheets-value='{"1":3,"3":-14}'>
				-14
			</td>
			<td data-sheets-value='{"1":3,"3":-28}'>
				-28
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2150.248640572143}'>
				2150
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1611.3070026126345}'>
				1611
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1182.3379794595003}'>
				1182
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":441.782320008762}'>
				442
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":241.8080928159956}'>
				242
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":560.4657347517474}'>
				560
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1010.7497546278173}'>
				1011
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4572.363150528281}'>
				4572
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5480.019272195351}'>
				5480
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6068.871578453591}'>
				6069
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5860.440467324999}'>
				5860
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6455.631652110662}'>
				6456
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5428.278789152926}'>
				5428
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":299.7823158958739}'>
				300
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4010.363141190181}'>
				4010
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5679.494073415938}'>
				5679
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5051.842176938296}'>
				5052
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5414.909076269363}'>
				5415
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"Shinovar coast"}'>
				Shinovar coast
			</td>
			<td data-sheets-value='{"1":3,"3":-14}'>
				-14
			</td>
			<td data-sheets-value='{"1":3,"3":-31}'>
				-31
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2383.6054400049493}'>
				2384
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1835.3539613696876}'>
				1835
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1328.5835630811396}'>
				1329
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":538.4095988912787}'>
				538
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":451.2265717183265}'>
				451
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":584.4811036801267}'>
				584
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1094.3886680996939}'>
				1094
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4758.841390519176}'>
				4759
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5681.95349702581}'>
				5682
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6301.149528597836}'>
				6301
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6113.225675816576}'>
				6113
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":6738.604052444343}'>
				6739
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5727.174053405646}'>
				5727
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":299.7823158958739}'>
				300
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4263.063270514405}'>
				4263
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5976.085802997031}'>
				5976
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5343.408047741236}'>
				5343
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5649.458752672314}'>
				5649
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"Dumadari"}'>
				Dumadari
			</td>
			<td data-sheets-value='{"1":3,"3":-21}'>
				-21
			</td>
			<td data-sheets-value='{"1":3,"3":15}'>
				15
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3744.959942275762}'>
				3745
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3849.2974550291287}'>
				3849
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4293.8248050778775}'>
				4294
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4252.701305710908}'>
				4253
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3812.2108975954025}'>
				3812
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3814.218735933745}'>
				3814
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3387.13354622867}'>
				3387
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1224.5019760935847}'>
				1225
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1703.890028038013}'>
				1704
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2087.7656197783763}'>
				2088
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1850.6282606268758}'>
				1851
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2586.4495882771007}'>
				2586
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2214.458183738257}'>
				2214
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4010.363141190181}'>
				4010
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4263.063270514405}'>
				4263
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2227.9228434784163}'>
				2228
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1551.4197623527396}'>
				1551
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1440.7786002780324}'>
				1441
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"E Akak"}'>
				E Akak
			</td>
			<td data-sheets-value='{"1":3,"3":-3}'>
				-3
			</td>
			<td data-sheets-value='{"1":3,"3":25}'>
				25
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4312.993189251954}'>
				4313
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4724.195759169973}'>
				4724
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5371.696462885674}'>
				5372
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5733.4259613913555}'>
				5733
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5555.475571592887}'>
				5555
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5699.201709309928}'>
				5699
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5385.917348448718}'>
				5386
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2873.0368653340424}'>
				2873
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2419.0077949282904}'>
				2419
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1906.7337564775014}'>
				1907
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1480.9294091021513}'>
				1481
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1010.3910426379607}'>
				1010
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":348.276915516745}'>
				348
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5679.494073415938}'>
				5679
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5976.085802997031}'>
				5976
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2227.9228434784163}'>
				2228
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":702.7981948502919}'>
				703
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1870.7970247361468}'>
				1871
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"Hearthstone"}'>
				Hearthstone
			</td>
			<td data-sheets-value='{"1":3,"3":-8}'>
				-8
			</td>
			<td data-sheets-value='{"1":3,"3":21}'>
				21
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":3921.6464770336092}'>
				3922
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4265.0415189585765}'>
				4265
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4880.663808707965}'>
				4881
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5149.687511046263}'>
				5150
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4910.6408725525}'>
				4911
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5029.239279167557}'>
				5029
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4696.141964939922}'>
				4696
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2360.9637145309625}'>
				2361
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2130.90437080479}'>
				2131
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1857.7752491486553}'>
				1858
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1409.10170616955}'>
				1409
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1443.504251756781}'>
				1444
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":671.5637845967167}'>
				672
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5051.842176938296}'>
				5052
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5343.408047741236}'>
				5343
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1551.4197623527396}'>
				1551
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":702.7981948502919}'>
				703
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1572.0845345436996}'>
				1572
			</td>
		</tr>
<tr>
<td data-sheets-value='{"1":2,"2":"Shattered Plains"}'>
				Shattered Plains
			</td>
			<td data-sheets-value='{"1":3,"3":-19}'>
				-19
			</td>
			<td data-sheets-value='{"1":3,"3":31}'>
				31
			</td>
			<td>
				 
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5066.1392375767955}'>
				5066
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5245.101615518784}'>
				5245
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5726.001845839667}'>
				5726
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5683.212879171529}'>
				5683
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5203.536526974893}'>
				5204
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5154.047912665552}'>
				5154
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":4683.3381975854645}'>
				4683
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1173.383416491995}'>
				1173
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":562.5970872363864}'>
				563
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":654.4251195379118}'>
				654
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":584.481103680127}'>
				584
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1575.9069595188241}'>
				1576
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":2092.918435320211}'>
				2093
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5414.909076269363}'>
				5415
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":5649.458752672314}'>
				5649
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1440.7786002780324}'>
				1441
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1870.7970247361468}'>
				1871
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":1572.0845345436996}'>
				1572
			</td>
			<td data-sheets-formula="=R28C2 * 2 * asin( sqrt(sin((R2C[0]*pi()/100-R[0]C2*pi()/100)/2)^2 + cos(R[0]C2*pi()/100) * cos(R2C[0]*pi()/100) * sin((R3C[0]*pi()/100-R[0]C3*pi()/100)/2)^2) )" data-sheets-numberformat='[null,2,"0",1]' data-sheets-value='{"1":3,"3":0}'>
				0
			</td>
		</tr>
</tbody>
</table>
]]></description><guid isPermaLink="false">635</guid><pubDate>Thu, 30 Aug 2018 04:35:00 +0000</pubDate></item><item><title>Roshar Physical Characteristics and Areas</title><link>https://www.17thshard.com/blogs/entry/634-roshar-physical-characteristics-and-areas/</link><description><![CDATA[
<p style="color:#1c1c1c">
	Some calculations I did a while back. Was planning to do more with the moons, but I just haven't had time and figured it was worth going ahead and posting this here as is.
</p>

<h2 style="color:#1c1c1c">
	Given
</h2>

<ol style="color:#1c1c1c">
	<li>
		<p>
			Surface gravity on Roshar is 0.7 g (source:<span> </span><em>Arcanum Unbounded</em>)
		</p>
	</li>
	<li>
		<p>
			Roshar's radius is 5663 km (source: <a href="https://wob.coppermind.net/events/332-jordancon-2018/#e10231" rel="external nofollow">JordanCon 2018</a>)
		</p>
	</li>
	<li>
		<p>
			<a href="https://coppermind.net/wiki/File:OB_Roshar.jpg" rel="external nofollow">This map of Roshar</a><span> </span>(minor WoR spioler) gives both latitude and longitude lines. The planet can be broken into 200 "squares" horizontally and 100 "squares" vertically. (source:<span> </span><a href="https://wob.coppermind.net/events/116/#e8890" rel="external nofollow">Peter on Reddit</a>)<span> </span><a href="https://www.brandonsanderson.com/wp-content/uploads/2019/11/twok_map-0_roshar-webres.jpg" rel="external nofollow">This map of Roshar</a><span> </span>(<a href="https://www.17thshard.com/topic/59890-roshar-map-reimagined/" rel="" style="color:#5e4473" target="_blank">an azumithal equidistant projection</a>) helps to place the equator as the latitude line passing through the southern tip of Kadrix island.
		</p>
	</li>
	<li>
		<p>
			One Rosharan solar day is 20 Rosharan hours. The moons have an orbital period of one solar day.
		</p>
	</li>
</ol>

<h2 style="color:#1c1c1c">
	Assumptions
</h2>

<ol style="color:#1c1c1c">
	<li>
		<p>
			The "standard cosmere" gravity is 1 g = 9.81 m/s<sup>2</sup><span> </span>(surface gravity on Earth)
		</p>
	</li>
	<li>
		<p>
			The "standard cosmere" size refers to planetary radius (and circumference) and is R = 6371 km (Earth's radius)
		</p>
	</li>
	<li>
		<p>
			The gravitational constant, G, remains unchanged
		</p>
	</li>
</ol>

<h2 style="color:#1c1c1c">
	Units
</h2>

<p style="color:#1c1c1c">
	Units are "real" units unless defined below.
</p>

<ol style="color:#1c1c1c">
	<li>
		<p>
			1 Rdeg (Rosharan degrees) = π/100 radians (200 Rdeg in a circle)
		</p>
	</li>
	<li>
		<p>
			1 Rhour (Rosharan hour) = 3473 seconds (<a href="https://www.17thshard.com/blogs/entry/633-rosharan-time-measurements/" rel="">calculation</a>)
		</p>
	</li>
</ol>

<h2 style="color:#1c1c1c">
	Calculations
</h2>

<h3 style="color:#1c1c1c">
	Size of Roshar (planet)
</h3>

<p style="color:#1c1c1c">
	Radius = 5663 km (88.8% of Earth  radius. This is roughly in line with Khriss's estimate that Roshar's radius is 0.9 R in <em>Arcanum Unbounded</em>.) 
</p>

<p style="color:#1c1c1c">
	Diameter = 11 330 km (88.8% of Earth diameter)
</p>

<p style="color:#1c1c1c">
	Circumference = 35 580 km (88.8% of Earth circumference)
</p>

<p style="color:#1c1c1c">
	Surface Area = 4 * π * (radius)<sup>2</sup><span> </span>= 4.030 × 10<sup>8</sup><span> </span>square km (79% of Earth surface area)
</p>

<p style="color:#1c1c1c">
	Volume = 4 / 3 * π * (radius)<sup>3</sup><span> </span>= 7.608 × 10<sup>11</sup><span> </span>cubic km (70% of Earth volume)
</p>

<h3 style="color:#1c1c1c">
	Mass Calculations
</h3>

<p style="color:#1c1c1c">
	Surface Gravity = 0.7 * g = 6.86 m/s<sup>2</sup><span> </span>(70% of Earth surface gravity)
</p>

<p style="color:#1c1c1c">
	Mass = (surface gravity) * (radius)<sup>2</sup><span> </span>/ G = 3.296×10<sup>24</sup><span> </span>kg (55% of Earth mass)
</p>

<p style="color:#1c1c1c">
	Density = mass / volume = 4.333 g/cm<sup>3</sup><span> </span>(79% of Earth density)
</p>

<h3 style="color:#1c1c1c">
	Characteristics of Roshar (continent)
</h3>

<p style="color:#1c1c1c">
	Northernmost point: northern tip of Iri @ 2 Rdeg N = 3.6 deg N
</p>

<p style="color:#1c1c1c">
	Including islands: northern tip of Kadrix island @ 3 Rdeg N = 5.4 deg N
</p>

<p style="color:#1c1c1c">
	Southernmost point: southern tip of Frostlands @ 30 Rdeg S = 54 deg S
</p>

<p style="color:#1c1c1c">
	Including islands: southern tip of Thaylenah @ 32 Rdeg S = 57.6 deg S
</p>

<p style="color:#1c1c1c">
	Easternmost point: New Natanan (and Frostlands coast) @ 37 Rdeg E = 66.6 deg E
</p>

<p style="color:#1c1c1c">
	Westernmost point: eastern tip of Steen @ 29 Rdeg W = 52.2 deg W
</p>

<p style="color:#1c1c1c">
	Including islands: eastern tip of Aimia @ 38 Rdeg W = 68.4 deg W
</p>

<p style="color:#1c1c1c">
	Furthest distance: west coast of Shinovar to tip of unclaimed NE peninsula = 10 610 km (<a href="https://www.17thshard.com/blogs/entry/635-roshar-distances/" rel="">calculation</a>)
</p>

<h3 style="color:#1c1c1c">
	Size Comparrisons
</h3>

<p style="color:#1c1c1c">
	By <a href="https://www.reddit.com/user/jofwu/comments/7ga3it/roshar_physical_calculations/dqhrh71/?context=8&amp;depth=9" rel="external nofollow">u/Shagomir on Reddit</a>, based on this <span style="color:#1c1c1c">Mollewide (equal-area) map:</span>
</p>

<p style="color:#1c1c1c">
	<img alt="8Z10QRk.png" class="ipsImage" height="501px" src="https://i.imgur.com/8Z10QRk.png" style="width: 500px; height: auto;" width="1000px">
</p>

<p style="color:#1c1c1c">
	Each pixel on the map is approximately 78.25 km<sup>2</sup>
</p>

<p style="color:#1c1c1c">
	Major regions:
</p>

<table style="color:#1c1c1c">
	<thead>
		<tr>
			<th>
				Region
			</th>
			<th>
				Area
			</th>
			<th>
				Comparison
			</th>
			<th>
				Area
			</th>
		</tr>
	</thead>
	<tbody>
		<tr>
			<td>
				Roshar (Total)
			</td>
			<td>
				414,030,000 km<sup>2</sup>
			</td>
			<td>
				Earth
			</td>
			<td>
				510,060,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Roshar Oceans
			</td>
			<td>
				373,780,000 km<sup>2</sup>
			</td>
			<td>
				Earth Oceans
			</td>
			<td>
				361,900,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Roshar (Continent)
			</td>
			<td>
				40,250,000 km<sup>2</sup>
			</td>
			<td>
				Asia
			</td>
			<td>
				43,820,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Aimia
			</td>
			<td>
				984,000 km<sup>2</sup>
			</td>
			<td>
				New Guinea
			</td>
			<td>
				786,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Thaylenah
			</td>
			<td>
				414,000 km<sup>2</sup>
			</td>
			<td>
				Sumatra
			</td>
			<td>
				443,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Purelake
			</td>
			<td>
				1,160,000 km<sup>2</sup>
			</td>
			<td>
				Caspian Sea
			</td>
			<td>
				371,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Sea of Spears
			</td>
			<td>
				129,000 km<sup>2</sup>
			</td>
			<td>
				Lake Superior
			</td>
			<td>
				82,100 km<sup>2</sup>
			</td>
		</tr>
	</tbody>
</table>

<p style="color:#1c1c1c">
	Size of countries:
</p>

<table style="color:#1c1c1c">
	<thead>
		<tr>
			<th>
				Region
			</th>
			<th>
				Area
			</th>
		</tr>
	</thead>
	<tbody>
		<tr>
			<td>
				Unclaimed
			</td>
			<td>
				8,649,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Alethkar
			</td>
			<td>
				7,134,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Jah Keved
			</td>
			<td>
				5,553,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Iri
			</td>
			<td>
				2,473,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Tu Bayla
			</td>
			<td>
				2,040,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Reshi Isles
			</td>
			<td>
				1,582,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Shinovar
			</td>
			<td>
				1,407,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Azir
			</td>
			<td>
				1,343,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Herdaz
			</td>
			<td>
				1,155,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Babatharnam
			</td>
			<td>
				1,107,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Rira
			</td>
			<td>
				1,056,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Aimia
			</td>
			<td>
				984,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Tukar
			</td>
			<td>
				702,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Emul
			</td>
			<td>
				596,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Marat
			</td>
			<td>
				524,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Greater Hexi
			</td>
			<td>
				454,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Thaylenah
			</td>
			<td>
				414,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Yezier
			</td>
			<td>
				396,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Marabethia
			</td>
			<td>
				394,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Yulay
			</td>
			<td>
				393,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Tashikk
			</td>
			<td>
				364,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Triax
			</td>
			<td>
				336,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Liafor
			</td>
			<td>
				319,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Desh
			</td>
			<td>
				230,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Steen
			</td>
			<td>
				156,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Alm
			</td>
			<td>
				144,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Bavland
			</td>
			<td>
				141,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Tu Fallia
			</td>
			<td>
				127,000 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				<em>Shattered Plains    </em>
			</td>
			<td>
				80,000 km<sup>2</sup>
			</td>
		</tr>
	</tbody>
</table>

<p style="color:#1c1c1c">
	List of comparable countries on Earth:
</p>

<table style="color:#1c1c1c">
	<thead>
		<tr>
			<th>
				Country
			</th>
			<th>
				Area
			</th>
		</tr>
	</thead>
	<tbody>
		<tr>
			<td>
				Russia
			</td>
			<td>
				16,377,742 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				United States
			</td>
			<td>
				9,147,593 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Australia
			</td>
			<td>
				7,633,565 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				India
			</td>
			<td>
				2,973,190 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Argentina
			</td>
			<td>
				2,736,690 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Mexico
			</td>
			<td>
				1,943,945 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Iran
			</td>
			<td>
				1,531,595 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				South Africa
			</td>
			<td>
				1,214,470 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Egypt
			</td>
			<td>
				995,450 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Turkey
			</td>
			<td>
				769,632 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Spain
			</td>
			<td>
				498,980 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Sweden
			</td>
			<td>
				410,335 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Germany
			</td>
			<td>
				348,672 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				United Kingdom
			</td>
			<td>
				241,930 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Syria
			</td>
			<td>
				183,630 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Iceland
			</td>
			<td>
				100,250 km<sup>2</sup>
			</td>
		</tr>
		<tr>
			<td>
				Czech Republic    
			</td>
			<td>
				77,247 km<sup>2</sup>
			</td>
		</tr>
	</tbody>
</table>

<h3 style="color:#1c1c1c">
	Moons
</h3>

<p style="color:#1c1c1c">
	Orbital period: T = 20 Rhours = 69 480 seconds (precession makes this weird)
</p>
]]></description><guid isPermaLink="false">634</guid><pubDate>Thu, 30 Aug 2018 04:23:00 +0000</pubDate></item><item><title>Rosharan Time Measurements</title><link>https://www.17thshard.com/blogs/entry/633-rosharan-time-measurements/</link><description><![CDATA[
<p>
	Roshar has <a href="https://www.17thshard.com/topic/6999-is-kaladin-actually-~27-years-old/#comment-115583" rel="">50 minutes/hour</a>, 20 hours/day, 5 days/week, 10 weeks/month (50-day months), 10 months/year (500-day years). Brandon and Peter have said that a Rosharan year is <a href="https://www.17thshard.com/topic/6999-is-kaladin-actually-~27-years-old/#comment-115583" rel="">1.10 Earth years</a> and that <a href="https://www.17thshard.com/topic/6999-is-kaladin-actually-~27-years-old/#comment-115487" rel="">a Rosharan hour is shorter than an Earth hour</a>. (This suggests we should assume the 1.10 number is precise.)
</p>

<p>
	The definition of a year is somewhat ambiguous. The Rosharan year above clearly refers to a solar year, so we will assume that the 1.10 number compares solar years. An Earth solar year is 365.24219 SI days of exactly 24 SI hours. So for Earth we'll use 60 minutes/hour, 24 hours/day, 7 days/week, 30 days/month, and 365.24219 days/year.
</p>

<p>
	---
</p>

<p>
	Using R to represent Roshar and E to represent Earth:
</p>

<p>
	1 R minute = 1.16 E minutes = 69.4 E seconds
</p>

<p>
	1 R hour = 0.964 E hours = 57.9 E minutes
</p>

<p>
	1 R day = 0.804 E days = 19.3 E hours
</p>

<p>
	1 R week = 0.574 E weeks = 4.02 E days
</p>

<p>
	1 R month = 1.34 E months = 40.2 E days
</p>

<p>
	1 R year = 1.10 E years = 13.4 E months = 402 E days
</p>

<p>
	---
</p>

<p>
	A 10 year-old Rosharan is 11 in Earth years.
</p>

<p>
	A 20 year-old Rosharan is 22 in Earth years.
</p>

<p>
	A 80 year-old Rosharan is 88 in Earth years.
</p>
]]></description><guid isPermaLink="false">633</guid><pubDate>Thu, 30 Aug 2018 03:33:00 +0000</pubDate></item></channel></rss>
