Problem
The hollow Moon. Newton proved that a sphere of uniform density attracts an external body as if all its mass were concentrated at the centre; he then extended the result to spherical shells of uniform density. Using these two results (and without resorting to integrals), show that a hollow sphere of outer radius , inner radius and total mass distributed uniformly in the shell attracts a body on its outer surface with exactly the same force as a solid sphere of equal mass and radius . Surprisingly the result does not depend on the inner radius : even a very thin “shell” of mass has the same effect.
Solution
Idea: shell as the difference of two solid spheres. As suggested, we think of the shell as the difference between a large solid sphere (radius ) and a small solid sphere (radius ), both with the same uniform density as the shell material. Subtracting the small one from the large one leaves exactly the hollow shell (Povey 2015, §10.1).
The masses of the two fictitious spheres. With common density :
Force on a body outside the surface (). A body of mass on the outer surface is at distance from the centre. It is external to both solid spheres, so by Newton’s theorem each acts as a point mass concentrated at the centre. The two forces are opposite (one attracts, the other is subtracted):
Conclusion. The force depends only on the total mass and the outer radius : identical to that of a solid sphere of equal mass. The surface acceleration is
Limiting case (thought experiment). In the limit the shell becomes an extremely thin cap: as long as the total mass is conserved, the density grows, but the external force remains . A “hollow Moon” would appear indistinguishable from a solid one, as long as we stay outside it.
Links
Topics: Gravitazione Concepts: Legge di gravitazione universale · Forza peso Skills: Impostazione simbolica · Analisi di casi limite e fantafisica