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Inverse-Square Law


An inverse-square law is a dependence f(r)=C/r^2 on the distance r>0 from a source, where C is independent of r. For a radial vector field in three-dimensional Euclidean space, suppose its radial component has spherical symmetry and its outward flux integral Phi is constant through concentric spheres. Since a sphere of radius r has surface area 4pir^2, the spherical symmetry gives

 F(r)=Phi/(4pir^2)r^^,

where r^^ is the outward radial unit vector (Staelin 2011, p. 18).

The divergence of this vector field is zero away from the source. For nonzero Phi, the flux integral through an enclosing sphere is consistent with the divergence theorem because the vector field has a singularity at the source. Thus the theorem cannot be applied there without accounting for the singularity.

More generally, in d-dimensional Euclidean space with d>=2, the corresponding radial law is

 F(r)=Phi/(A_(d-1)r^(d-1))r^^,

where A_(d-1)=2pi^(d/2)/Gamma(d/2) is the hyper-surface area of the unit hypersphere, and Gamma is the gamma function. When Phi!=0, the inverse-square case is therefore specific to three dimensions. The gravitational inverse-square law is the hypothesis underlying Newton's shell theorem.


See also

Flux Integral, Newton's Shell Theorem

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References

Staelin, D. H. "Gauss's Law and Electrostatic Fields and Potentials." §1.3 in Electromagnetics and Applications. Cambridge, MA: Massachusetts Institute of Technology, pp. 17-20, 2011. https://ocw.mit.edu/courses/6-013-electromagnetics-and-applications-spring-2009/d3be4ea78b036a6362230fb41780cf54_MIT6_013S09_notes.pdf.

Cite this as:

Weisstein, Eric W. "Inverse-Square Law." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/Inverse-SquareLaw.html

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