| Assumptions:
1) Earth is a sphere with radius r
2) "Sky" is a hollow spherical shell with radius R The surface area of the entire spherical sky is: 4\piR^2 This can be represented by a spherical integral that I'm not sure I can write cleanly here. We just need to change the bounds of that integral to find the area of the observable part of that shell. The Intersecting Chord Theorem along with some trigonometry can be used to find these bounds. The answer I get is: (1 - cos(x)) / 2 where x = Arctan(sqrt(r(R-r)) / r) This seems to have the correct asymptotic behavior (as r approaches 0, cos(x) approaches cos(pi/2) = 0, and the answer approaches 50% EDIT: My previous answer assumed the shapes were cones instead of spheres. Sorry about the confusion. |