Homoeoid and focaloid

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A homoeoid or homeoid is a shell (a bounded region) bounded by two concentric, similar ellipses (in 2D) or ellipsoids (in 3D).[1][2] When the thickness of the shell becomes negligible, it is called a thin homoeoid. The name homoeoid was coined by Lord Kelvin and Peter Tait.[3] Closely related is the focaloid, a shell between concentric, confocal ellipses or ellipsoids.[4]

Cut view of a homoeoid in 3D
Cut view of a focaloid in 3D

Mathematical definition

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If the outer shell is given by

 

with semiaxes  , the inner shell of a homoeoid is given for   by

 

and a focaloid is defined for   by

 

The thin homoeoid is then given by the limit  , and the thin focaloid is the limit  .[3]

Physical properties

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Thin focaloids and homoeoids can be used as elements of an ellipsoidal matter or charge distribution that generalize the shell theorem for spherical shells. The gravitational or electromagnetic potential of a homoeoid homogeneously filled with matter or charge is constant inside the shell, so there is no force on a test particle inside of it.[5] Meanwhile, two uniform, concentric focaloids with the same mass or charge exert the same potential on a test particle outside of both.[4][1]

See also

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References

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  1. ^ a b Chandrasekhar, S.: Ellipsoidal Figures of Equilibrium, Yale Univ. Press. London (1969)
  2. ^ Routh, E. J.: A Treatise on Analytical Statics, Vol II, Cambridge University Press, Cambridge (1882)
  3. ^ a b Harry Bateman. "Partial differential equations of mathematical physics.", Cambridge, UK: Cambridge University Press, 1932 (1932).
  4. ^ a b Rodrigues, Hilário (11 May 2014). "On determining the kinetic content of ellipsoidal configurations". Monthly Notices of the Royal Astronomical Society. 440 (2): 1519–1526. arXiv:1402.6541. doi:10.1093/mnras/stu353.
  5. ^ Michel Chasles, Solution nouvelle du problème de l’attraction d’un ellipsoïde hétérogène sur un point exterieur, Jour. Liouville 5, 465–488 (1840)
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