An alternative method to construct a consistent second-order theory on the equilibrium figures of rotating celestial bodies
Autor: | Miguel Barreda Rochera, José Antonio López Ortí, Manuel Forner Gumbau |
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Rok vydání: | 2022 |
Předmět: |
Mass distribution
Applied Mathematics Equipotential surface Mathematical analysis Coordinate system computational algebra figures of rotating celestial bodies spherical harmonics Spherical coordinate system Angular velocity 010103 numerical & computational mathematics 01 natural sciences potential theory 010101 applied mathematics Computational Mathematics Equipotential Center of mass 0101 mathematics Laplace operator perturbation theory Mathematics |
Zdroj: | Repositori Universitat Jaume I Universitat Jaume I |
ISSN: | 0377-0427 |
DOI: | 10.1016/j.cam.2020.113305 |
Popis: | The main objective of this work is to construct a new method to develop a consistent second-order amplitudes theory to evaluate the potential of a rotating deformable celestial body when the hydrostatic system equilibrium has been achieved. In this case, we have: ∇ P = ρ ∇ Ψ , △ Ψ = − 4 π G ρ + 2 ω 2 , where P is the pressure, ρ is the density, Ψ is the total potential, △ is Laplace operator, G is the gravitational constant and ω is the angular velocity of the system. To integrate these equations in a general case of mass distribution a state equation relating pressure and density is needed. To assess the full potential, Ψ , it is necessary to calculate the self-gravitational potential, Ω , and the centrifugal potential, V c . The equilibrium configuration involves the hydrostatic equilibrium, it is, the rigid rotation of the system corresponding to the minimum potential and, according to Kopal, this state involves the identification of equipotential, isobaric, isothermal and isopycnic surfaces. To study the structure of the body we define a coordinate system O X Y Z where O is the center of mass of the component, O X is an axis fixed in an arbitrary point of the body equator, O Z an axis parallel to angular velocity ω → and O Y defining a direct trihedron. For an arbitrary point P in the rotating body the Clairaut coordinates are given by ( a , θ , λ ) where a is the radius of the sphere that contains the same mass that the equipotential surface that contains P and ( θ , λ ) are the angular spherical coordinates of P . This problem has been solved in the first order in ω 2 following two techniques: the first one is based on the asymptotic properties of the numerical quadrature formulae. The second is similar to the one used by Laplace to develop the inverse of the distance between two planets. The second-order theory based on the first method has been developed by the authors in a recent paper. In this work we develop a consistent second-order theory about the equilibrium figures of rotating celestial bodies based on the second method. Finally, to show the performance of the method it is interesting to study a numerical example based on a convective star. |
Databáze: | OpenAIRE |
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