The shell theorem, proved by Isaac Newton, is a result in classical mechanics that simplifies the gravitational effect of a spherically symmetric body. It states that such a body attracts objects outside it exactly as if all of its mass were concentrated at a single point at its center, and that a spherically symmetric hollow shell exerts no net gravitational force at all on an object located anywhere inside it. A consequence of these two facts is that, inside a solid sphere of uniform density, the gravitational force on an object varies in direct proportion to its distance from the center, falling to zero exactly at the center of mass. The theorem is applied throughout astronomy whenever the gravitational effect of a star, planet, or other roughly spherical body needs to be calculated.
Facts
StatementA spherically symmetric body affects external objects gravitationally as though all of its mass were concentrated at a point at its center, and a spherically symmetric shell exerts no net gravitational force on any object inside it. 1 Classification
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Source Shell theorem, Wikipedia
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Source Shell theorem, Wikipedia
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1. Shell theorem, Wikipedia
Statement section, first point
A spherically symmetric body affects external objects gravitationally as though all of its mass were concentrated at a point at its center.
References
Newton, Isaac (1687). Philosophiae Naturalis Principia Mathematica. London. pp. 193, Theorem XXXI.
Proved By: Isaac Newton, Lead
Isaac Newton proved the shell theorem and stated that:
In Group: Classical Mechanics and Dynamics, Lead section
In classical mechanics, the shell theorem gives gravitational simplifications
In Branch: Mathematical Physics, Lead section
In classical mechanics, the shell theorem gives gravitational simplifications
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