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tidal tensor : ウィキペディア英語版
tidal tensor

In Newton's theory of gravitation and in various relativistic classical theories of gravitation, such as general relativity, the tidal tensor represents
#''tidal accelerations'' of a cloud of (electrically neutral, nonspinning) test particles,
#''tidal stresses'' in a small object immersed in an ambient gravitational field.
==Newton's theory==
In the field theoretic elaboration of ''Newtonian gravity'', the central quantity is the gravitational potential U, which obeys the Poisson equation
:\Delta U = 4 \pi \, \mu
where \mu is the mass density of any matter present. Note that this equation implies that in a vacuum solution, the potential is simply a harmonic function.
The ''tidal tensor'' is given by the ''traceless part''
:\Phi_ = J_ - \frac \, _m \, \eta_
of the Hessian
: J_ = \frac
where we are using the standard ''Cartesian chart'' for E3, with the Euclidean metric tensor
: ds^2 = dx^2 + dy^2 + dz^2, \; -\infty < x,y,z < \infty
Using standard results in vector calculus, this is readily converted to expressions valid in other coordinate charts, such as the ''polar spherical chart''
: ds^2 = d\rho^2 + \rho^2 \, \left( d\theta^2 + \sin(\theta)^2 \, d\phi^2 \right)
: 0 < \rho < \infty, \; 0 < \theta < \pi, \; -\pi < \phi < \pi

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「tidal tensor」の詳細全文を読む



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