Dirichlet's ellipsoidal problem

In astrophysics, Dirichlet's ellipsoidal problem, named after Peter Gustav Lejeune Dirichlet, asks under what conditions there can exist an ellipsoidal configuration at all times of a homogeneous rotating fluid mass in which the motion, in an inertial frame, is a linear function of the coordinates. Dirichlet's basic idea was to reduce Euler equations to a system of ordinary differential equations such that the position of a fluid particle in a homogeneous ellipsoid at any time is a linear and homogeneous function of initial position of the fluid particle, using Lagrangian framework instead of the Eulerian framework.[1][2][3]

  1. ^ Chandrasekhar, S. (1969). Ellipsoidal figures of equilibrium (Vol. 10, p. 253). New Haven: Yale University Press.
  2. ^ Chandrasekhar, S. (1967). Ellipsoidal figures of equilibrium—an historical account. Communications on Pure and Applied Mathematics, 20(2), 251–265.
  3. ^ Lebovitz, N. R. (1998). The mathematical development of the classical ellipsoids. International journal of engineering science, 36(12), 1407–1420.

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