Is Gauss' Law Applicable to Gravitational Fields?

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Gauss' Law can be applied to gravitational fields similarly to how it is used in electrostatics. The gravitational field equations mirror those of electrostatics, with gravitational force corresponding to electric force through specific constants. In integral form, Gauss' Law for gravity can be expressed as the surface integral of the gravitational field equating to the enclosed mass multiplied by a constant. The differential form also shows a direct relationship between the divergence of the gravitational field and mass density. Thus, Gauss' Law is indeed applicable to gravitational fields, demonstrating the parallels between gravitational and electrostatic phenomena.
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Can gauss law in its equivalent form be used to determine the gravitational field??

If so how??
 
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Yes. Notice how gravity corresponds with electrostatics; for point masses/charges you have
\vec E = \frac{1}{4\pi\epsilon_0} \frac{q}{r^2} \hat r \leftrightarrow \vec g = -G \frac{m}{r^2} \hat r.
Thus you have the correspondences q \leftrightarrow m, 1/4\pi\epsilon_0 \leftrightarrow -G.

From Gauss's law (in integral form) for electrostatics, you can get the corresponding equation for gravity:
<br /> \oint \vec E \cdot d \vec a = \frac{q_{encl}}{\epsilon_0}<br /> \leftrightarrow<br /> \oint \vec g \cdot d \vec a = -4\pi Gm_{encl}.<br />
In differential form you get
<br /> \nabla \cdot \vec E = \frac{\rho_e}{\epsilon_0}<br /> \leftrightarrow<br /> \nabla \cdot \vec g = -4\pi G \rho_m<br />
where \rho_e is the charge density, and \rho_m is the mass density.
 
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