Shell theorem: Difference between revisions

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Changing short description from "Statement on the gravitational attraction of spherical bodies." to "Statement on the gravitational attraction of spherical bodies"
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:<math>\int_S {\mathbf g}\cdot \,d{\mathbf {S}} = \int_S {\mathbf g}\cdot {\hat\mathbf{n}}\,dS</math>
is the [[surface integral]] of the [[gravitational field]] '''<math>\mathbf{g'''}</math> over any [[closed surface]] inside which the total mass is ''M'', the [[unit vector]] <math>\hat\mathbf{n}</math> being the outward normal to the surface.
 
The gravitational field of a spherically symmetric mass distribution like a mass point, a spherical shell or a homogeneous sphere must also be spherically symmetric. If <math>\hat\mathbf{n}</math> is a unit vector in the direction from the point of symmetry to another point the gravitational field at this other point must therefore be