Imagine a sphere being one's eyeball and the rectangular area being the picture of one's view. Like putting a name tag sticker on a balloon. How can I find the area of the rectangle on the sphere?
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homework question? – Loreno Heer Nov 09 '14 at 21:55
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3There's no such thing as a rectangle on a sphere -- the sum of angles in a spherical quadrilateral always exceeds 360°, so the angles can't all be right. – hmakholm left over Monica Nov 09 '14 at 21:56
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Could you perhaps provide an explaining sketch? – flawr Nov 09 '14 at 21:57
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Area of a Latitude-Longitude Rectangle – Nov 09 '14 at 22:48
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Of course you can’t put a name tag on a balloon, because you would be making it crimp as you stuck it on. We need much more information. How do you describe your rectangle? By its vertices? By the lengths of its sides? By its height and its width? (This is not the same as the previous!) Are its sides “straight”, i.e. are its sides what you would get by looking at a straight line hanging in space? The lines of latitude, parallel to the equator, are not “straight” in this sense, i.e. they are not geodesics. – Lubin Nov 10 '14 at 18:44
2 Answers
You need to define a spherical rectangle. There is no figure on a sphere with four sides, each a segment of a great circle (a straight line on the sphere) and with four right angles.
A plane rectangle has opposite sides equal in length and all angles equal. So, let's define a spherical rectangle in the same way:
Definition: a rectangle on the sphere is a four-sided polygon with opposite sides having equal length and all four internal angles of equal magnitude.
For example, take the two meridians on the globe at longitude +15 deg and -15 deg. Join the points at latitude +20 deg on each meridian by a great circle segment (straight line). Do the same for the points at latitude -20 deg on each meridian. Voila: we have a spherical rectangle.
To get the area, draw either diagonal, calculate the area of either resulting triangle and double the value.
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Presumably if your angle at the four vertices is $\alpha$, then your area is $4\alpha-2\pi$? – Lubin Nov 10 '14 at 18:06
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Yes. Each triangle has area equal to angular excess $2\alpha-\pi$ which gives its area (we assume sphere has unit radius). Thus, as Lubin says, area of rectangle is $4\alpha-2\pi$. – Rocky Nov 10 '14 at 19:40
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Ok great answers, but still having trouble comprehending this. I guess some background information would help. Imagine I am looking at a picture, or tv on a wall. The dimensions of my vision are this "sticker on a balloon" or spherical "rectangle" I'm asking about. So the tv remains the same dimensions, but my visual dimensions change as I get closer/farther. I'm looking to maximize the size of this "rectangle" while not compromising the vertical angle (I know if we get closer and closer the horizontal angle becomes greater and greater) I want to maximize both angles and the rectangle. – Mathlete Nov 10 '14 at 20:01
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This goes beyond mathematics. Light from the TV will pass through the lens (which we might take as a point) and hit the retina. It is not clear that a line (the edge of the TV screen projects to a great circle. – Rocky Nov 10 '14 at 21:37
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Since the edges of the picture are straight lines, your “rectangle” is unquestionably bounded by geodesics. I’ll give a solution based on inputs that make the calculation comparatively easy. Soon. – Lubin Nov 11 '14 at 00:41
Let’s describe your “rectangle” this way:
Think of your figure as centered on the point $0$ longitude, $0$ latitude, extending upwards and downwards by $\alpha$ and to the right and to the left by $\beta$. These are angles, as you realize. Now the top side is perpendicular to the vertical line segment, similarly the bottom side. In the same way, the left and right sides are perpendicular to the horizontal line. We need look only at the upper left quadrangle, which has three right angles and an unknown angle $C$, whose size we need to evaluate, as @Rocky pointed out in his response.
It’s now a question of spherical trigonometry, which seems to have been understood already by Napier, who died a quarter-century before Newton’s birth. The first task is to find the length of the segment I’ve labeled $\gamma$, and that’s nicely given by the Spherical Pythagorean Theorem, it says $\cos\gamma=\cos\alpha\cos\beta$. We also need the angles $A$ and $B$, and they’re given by another of Napier’s rules for spherical right triangles, namely that $\tan(\text{angle})=\tan(\text{opposite})/\sin(\text{adjacent})$, so that here, $\tan A=\tan\alpha/\sin\beta$, and similarly, $\tan B=\tan\beta/\sin\alpha$.
Of course it’s the complements of these angles that we want for solving the triangle containing the angle $C$, I’ll call them $\bar A$ and $\bar B$. But $\tan A=\cot \bar A=1/\tan \bar A$. Thus we have the relations $\tan\bar A=\sin\beta\cot\alpha$, $\tan\bar B=\sin\alpha\cot\beta$. You can express $\bar A$ and $\bar B$ as the values of the inverse tangent function, if you like.
Now finally, we have a triangle with data of ASA type, and for this you use the Dual Law of Cosines, which says, for a triangle labeled in the standard way with angles $A$, $B$, and $C$ with opposite sides $a$, $b$, and $c$ respectively, that $$ \cos C=-\cos A\cos B +\sin A\sin B\cos c\,. $$ For our data, replace $A$ with $\bar A$, $B$ with $\bar B$, and $c$ with $\gamma$. We do have the previous fact that $\cos\gamma=\cos\alpha\cos\beta$.
Let’s do a representative example. Suppose our rectangle extends $20^\circ$ top to bottom and $40^\circ$ left to right, so that $\alpha=10^\circ$ and $\beta=20^\circ$. Then $\gamma=\arccos(\cos10^\circ\cos20^\circ)=22.2687^\circ$. Continuing, $\bar A=\arctan(\sin20^\circ/\tan10^\circ)=62.7268^\circ$ and $\bar B=\arctan\sin10^\circ/\tan20^\circ=25.5056^\circ$. Finally, \begin{align} C&=\arccos(\sin62.7268^\circ\sin25.5056^\circ\cos22.2687^\circ -\cos62.7268^\circ\cos25.5056^\circ)\\ &=93.4049^\circ \end{align} Now we muliply by $4$ and subtract $360^\circ$, then convert to radians, getting $.2377$, and to get an area quantity, multiply by $r^2$, the radius of your sphere, in other words the distance to the center of your picture.
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