As I see it;
The energy distribution should go as R^3, where R is the distance to the point of detonation.
If this point is in the air, we could ask how the distribtion looks as seen from the point on the ground above which the nuke is detonated (the projection of the sphere unto a surface) then the distribution should go like (h^2+r^2)^(3/2), where h is the height of the detonation above the surface and and r is the distance from the perpendicular projection of the point of detonation unto the surface.
So seen on a map, the destruction is more concentrated around the center than a cubic decrease. Though a distance (r>>h) from the center you have a cubic decrease.
The energy distribution should go as R^3, where R is the distance to the point of detonation.
If this point is in the air, we could ask how the distribtion looks as seen from the point on the ground above which the nuke is detonated (the projection of the sphere unto a surface) then the distribution should go like (h^2+r^2)^(3/2), where h is the height of the detonation above the surface and and r is the distance from the perpendicular projection of the point of detonation unto the surface.
So seen on a map, the destruction is more concentrated around the center than a cubic decrease. Though a distance (r>>h) from the center you have a cubic decrease.
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