请输入您要查询的百科知识:

 

词条 Maclaurin spheroid
释义

  1. Maclaurin formula

  2. Stability

  3. See also

  4. References

A Maclaurin spheroid is an oblate spheroid which arises when a self-gravitating fluid body of uniform density rotates with a constant angular velocity. This spheroid is named after the Scottish mathematician Colin Maclaurin, who formulated it for the shape of Earth in 1742.[1] In fact the figure of the Earth is far less oblate than this, since the Earth is not homogeneous, but has a dense iron core. The Maclaurin spheroid is considered to be the simplest model of rotating ellipsoidal figures in equilibrium since it assumes uniform density.

Maclaurin formula

For spheroid with semi-major axis and semi-minor axis , the angular velocity is given by the Maclaurin's formula[2]

where is the eccentricity of meridional cross-sections of the spheriod, is the density and is the Gravitational constant. The formula predicts two possible types of equilibrium figures when , one is a sphere () and the other is a flattened spheroid (). The maximum angular velocity occurs at eccentricity and its value is , so that above this speed, no equilibrium figures exist. The angular momentum is

where is the mass of the spheroid and is the mean radius, the radius of a sphere of the same volume as the spheroid.

Stability

For a Maclaurin spheroid of eccentricity greater than 0.812670, a Jacobi ellipsoid of the same angular momentum has lower total energy. If such a spheroid is composed of a viscous fluid, and if it suffers a perturbation which breaks its rotational symmetry, then it will gradually elongate into the Jacobi ellipsoidal form, while dissipating its excess energy as heat. This is termed secular instability. However, for a similar spheroid composed of an inviscid fluid, the perturbation will merely result in an undamped oscillation. This is described as dynamic (or ordinary) stability.

A Maclaurin spheroid of eccentricity greater than 0.952887 is dynamically unstable. Even if it is composed of an inviscid fluid and has no means of losing energy, a suitable perturbation will grow (at least initially) exponentially. Dynamic instability implies secular instability (and secular stability implies dynamic stability).[5]

See also

  • Jacobi ellipsoid
  • Spheroid
  • Ellipsoid

References

1. ^Maclaurin, Colin. A Treatise of Fluxions: In Two Books. 1. Vol. 1. Ruddimans, 1742.
2. ^Chandrasekhar, Subrahmanyan. Ellipsoidal figures of equilibrium. Vol. 10. New Haven: Yale University Press, 1969.
3. ^{{cite book |last1 = Lyttleton |first1 = Raymond Arthur |author-link1 = Raymond Lyttleton |title = The Stability Of Rotating Liquid Masses |year = 1953 |publisher = Cambridge University Press |isbn = 9781316529911 |url = https://archive.org/details/stabilityofrotat032172mbp }}
[3]
}}

3 : Quadrics|Astrophysics|Fluid dynamics

随便看

 

开放百科全书收录14589846条英语、德语、日语等多语种百科知识,基本涵盖了大多数领域的百科知识,是一部内容自由、开放的电子版国际百科全书。

 

Copyright © 2023 OENC.NET All Rights Reserved
京ICP备2021023879号 更新时间:2024/9/27 5:41:16