What Are the Radial and Tangential Accelerations in the Kerr Metric?

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SUMMARY

The discussion focuses on the radial and tangential gravitational accelerations of a moving particle in Schwarzschild coordinates, specifically represented by the equations for v_r and v_\phi. Users seek an equivalent set of equations for the Kerr metric, particularly for movement along the equator of a rotating black hole. A referenced paper by Donato Bini et al. explores gravitational acceleration in the Kerr metric, detailing the influence of gravitoelectromagnetic fields and the behavior of parallel transport in circular orbits. This analysis extends the understanding of 4-acceleration in the context of the Kerr spacetime.

PREREQUISITES
  • Understanding of Schwarzschild coordinates and their applications
  • Familiarity with the Kerr metric and its implications in general relativity
  • Knowledge of gravitational acceleration equations in curved spacetime
  • Basic grasp of parallel transport and Lorentz transformations in physics
NEXT STEPS
  • Study the equations of motion in the Kerr metric for circular orbits
  • Examine the paper "Geometric transport along circular orbits in stationary axisymmetric spacetimes" by Donato Bini et al.
  • Research the effects of gravitoelectromagnetic fields on particle motion in rotating black holes
  • Learn about the Frenet-Serret parameters and their role in circular orbits in general relativity
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Researchers in theoretical physics, astrophysicists studying black hole dynamics, and students of general relativity seeking to deepen their understanding of gravitational effects in rotating spacetimes.

Jorrie
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Pervect has https://www.physicsforums.com/showpost.php?p=1046874&postcount=17" for radial and tangential gravitational accelerations of a moving particle in Schwarzschild coordinates.

[tex] \frac{d^2 r}{d t^2} = \frac {3 m{{\it v_r}}^{2}}{ \left( r-2\,m \right) r} + \left( r-2\,m \right) \left( {{\it v_\phi}}^{2}-{\frac {m}{{r}^{3}}} \right) [/tex]

[tex] \frac{d^2\phi}{d t^2} = -\frac {2 {\it v_r}\,{\it v_\phi}\, \left( r -3\,m \right) }{ \left( r-2\,m \right) r}[/tex]

where [itex]v_r =dr/dt[/itex], [itex]v_\phi = d\phi/dt[/itex], [itex]m[/itex] the mass of the primary and [itex]r,\phi[/itex] the Schwarzschild coordinate parameters.

Does anyone know of an equivalent set of equations for the Kerr metric, at least for movement along the equator of a rotating black hole?
 
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I know that this is a seriously old thread but it remains unanswered. The following paper looks at gravitational acceleration for moving objects in Kerr metric-

http://arxiv.org/abs/gr-qc/0407004

'Geometric transport along circular orbits in stationary axisymmetric spacetimes'

Donato Bini, Christian Cherubini, Gianluca Cruciani, Robert T. Jantzen

(Submitted on 1 Jul 2004)

'Parallel transport along circular orbits in orthogonally transitive stationary axisymmetric spacetimes is described explicitly relative to Lie transport in terms of the electric and magnetic parts of the induced connection. The influence of both the gravitoelectromagnetic fields associated with the zero angular momentum observers and of the Frenet-Serret parameters of these orbits as a function of their angular velocity is seen on the behavior of parallel transport through its representation as a parameter-dependent Lorentz transformation between these two inner-product preserving transports which is generated by the induced connection. This extends the analysis of parallel transport in the equatorial plane of the Kerr spacetime to the entire spacetime outside the black hole horizon, and helps give an intuitive picture of how competing "central attraction forces" and centripetal accelerations contribute with gravitomagnetic effects to explain the behavior of the 4-acceleration of circular orbits in that spacetime.'
 
Thanks Steve, it looks promising!
 

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