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Mathisson–Papapetrou–Dixon equations

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General relativity equation
General relativity
Spacetime curvature schematic
G μ ν + Λ g μ ν = κ T μ ν {\displaystyle G_{\mu \nu }+\Lambda g_{\mu \nu }={\kappa }T_{\mu \nu }} {\displaystyle G_{\mu \nu }+\Lambda g_{\mu \nu }={\kappa }T_{\mu \nu }}

In physics, specifically general relativity, the Mathisson–Papapetrou–Dixon equations describe the motion of a massive spinning body moving in a gravitational field. Other equations with similar names and mathematical forms are the Mathisson–Papapetrou equations and Papapetrou–Dixon equations. All three sets of equations describe the same physics.

These equations are named after Myron Mathisson,[1] William Graham Dixon,[2] and Achilles Papapetrou,[3] who worked on them.

Throughout, this article uses the natural units c = G = 1, and tensor index notation.

Mathisson–Papapetrou–Dixon equations

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The Mathisson–Papapetrou–Dixon (MPD) equations for a mass m {\displaystyle m} {\displaystyle m} spinning body are

D k ν D τ + 1 2 S λ μ R λ μ ν ρ V ρ = 0 , D S λ μ D τ + V λ k μ − V μ k λ = 0. {\displaystyle {\begin{aligned}{\frac {Dk_{\nu }}{D\tau }}+{\frac {1}{2}}S^{\lambda \mu }R_{\lambda \mu \nu \rho }V^{\rho }&=0,\\{\frac {DS^{\lambda \mu }}{D\tau }}+V^{\lambda }k^{\mu }-V^{\mu }k^{\lambda }&=0.\end{aligned}}} {\displaystyle {\begin{aligned}{\frac {Dk_{\nu }}{D\tau }}+{\frac {1}{2}}S^{\lambda \mu }R_{\lambda \mu \nu \rho }V^{\rho }&=0,\\{\frac {DS^{\lambda \mu }}{D\tau }}+V^{\lambda }k^{\mu }-V^{\mu }k^{\lambda }&=0.\end{aligned}}}

Here τ {\displaystyle \tau } {\displaystyle \tau } is the proper time along the trajectory, k ν {\displaystyle k_{\nu }} {\displaystyle k_{\nu }} is the body's four-momentum

k ν = ∫ t = const T 0 ν g d 3 x , {\displaystyle k_{\nu }=\int _{t={\text{const}}}{T^{0}}_{\nu }{\sqrt {g}}d^{3}x,} {\displaystyle k_{\nu }=\int _{t={\text{const}}}{T^{0}}_{\nu }{\sqrt {g}}d^{3}x,}

the vector V μ {\displaystyle V^{\mu }} {\displaystyle V^{\mu }} is the four-velocity of some reference point X μ {\displaystyle X^{\mu }} {\displaystyle X^{\mu }} in the body, and the skew-symmetric tensor S μ ν {\displaystyle S^{\mu \nu }} {\displaystyle S^{\mu \nu }} is the angular momentum

S μ ν = ∫ t = const { ( x μ − X μ ) T 0 ν − ( x ν − X ν ) T 0 μ } g d 3 x {\displaystyle S^{\mu \nu }=\int _{t={\text{const}}}\left\{\left(x^{\mu }-X^{\mu }\right)T^{0\nu }-\left(x^{\nu }-X^{\nu }\right)T^{0\mu }\right\}{\sqrt {g}}d^{3}x} {\displaystyle S^{\mu \nu }=\int _{t={\text{const}}}\left\{\left(x^{\mu }-X^{\mu }\right)T^{0\nu }-\left(x^{\nu }-X^{\nu }\right)T^{0\mu }\right\}{\sqrt {g}}d^{3}x}

of the body about this point. In the time-slice integrals we are assuming that the body is compact enough that we can use flat coordinates within the body where the energy-momentum tensor T μ ν {\displaystyle T^{\mu \nu }} {\displaystyle T^{\mu \nu }} is non-zero.

As they stand, there are only ten equations to determine thirteen quantities. These quantities are the six components of S λ μ {\displaystyle S^{\lambda \mu }} {\displaystyle S^{\lambda \mu }}, the four components of k ν {\displaystyle k_{\nu }} {\displaystyle k_{\nu }} and the three independent components of V μ {\displaystyle V^{\mu }} {\displaystyle V^{\mu }}. The equations must therefore be supplemented by three additional constraints which serve to determine which point in the body has velocity V μ {\displaystyle V^{\mu }} {\displaystyle V^{\mu }}. Mathison and Pirani originally chose to impose the condition V μ S μ ν = 0 {\displaystyle V^{\mu }S_{\mu \nu }=0} {\displaystyle V^{\mu }S_{\mu \nu }=0} which, although involving four components, contains only three constraints because V μ S μ ν V ν {\displaystyle V^{\mu }S_{\mu \nu }V^{\nu }} {\displaystyle V^{\mu }S_{\mu \nu }V^{\nu }} is identically zero. This condition, however, does not lead to a unique solution and can give rise to the mysterious "helical motions".[4] The Tulczyjew–Dixon condition k μ S μ ν = 0 {\displaystyle k_{\mu }S^{\mu \nu }=0} {\displaystyle k_{\mu }S^{\mu \nu }=0} does lead to a unique solution as it selects the reference point X μ {\displaystyle X^{\mu }} {\displaystyle X^{\mu }} to be the body's center of mass in the frame in which its momentum is ( k 0 , k 1 , k 2 , k 3 ) = ( m , 0 , 0 , 0 ) {\displaystyle (k_{0},k_{1},k_{2},k_{3})=(m,0,0,0)} {\displaystyle (k_{0},k_{1},k_{2},k_{3})=(m,0,0,0)}.

Accepting the Tulczyjew–Dixon condition k μ S μ ν = 0 {\displaystyle k_{\mu }S^{\mu \nu }=0} {\displaystyle k_{\mu }S^{\mu \nu }=0}, we can manipulate the second of the MPD equations into the form

D S λ μ D τ + 1 m 2 ( S λ ρ k μ D k ρ D τ + S ρ μ k λ D k ρ D τ ) = 0 , {\displaystyle {\frac {DS_{\lambda \mu }}{D\tau }}+{\frac {1}{m^{2}}}\left(S_{\lambda \rho }k_{\mu }{\frac {Dk^{\rho }}{D\tau }}+S_{\rho \mu }k_{\lambda }{\frac {Dk^{\rho }}{D\tau }}\right)=0,} {\displaystyle {\frac {DS_{\lambda \mu }}{D\tau }}+{\frac {1}{m^{2}}}\left(S_{\lambda \rho }k_{\mu }{\frac {Dk^{\rho }}{D\tau }}+S_{\rho \mu }k_{\lambda }{\frac {Dk^{\rho }}{D\tau }}\right)=0,}

This is a form of Fermi–Walker transport of the spin tensor along the trajectory – but one preserving orthogonality to the momentum vector k μ {\displaystyle k^{\mu }} {\displaystyle k^{\mu }} rather than to the tangent vector V μ = d X μ / d τ {\displaystyle V^{\mu }=dX^{\mu }/d\tau } {\displaystyle V^{\mu }=dX^{\mu }/d\tau }. Dixon calls this M-transport.

See also

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References

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Notes

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  1. ^ M. Mathisson (1937). "Neue Mechanik materieller Systeme". Acta Physica Polonica. Vol. 6. pp. 163–209.
  2. ^ W. G. Dixon (1970). "Dynamics of Extended Bodies in General Relativity. I. Momentum and Angular Momentum". Proc. R. Soc. Lond. A. 314 (1519): 499–527. Bibcode:1970RSPSA.314..499D. doi:10.1098/rspa.1970.0020. S2CID 119632715.
  3. ^ A. Papapetrou (1951). "Spinning Test-Particles in General Relativity. I". Proc. R. Soc. Lond. A. 209 (1097): 248–258. Bibcode:1951RSPSA.209..248P. doi:10.1098/rspa.1951.0200. S2CID 121464697.
  4. ^ L. F. O. Costa; J. Natário; M. Zilhão (2012). "Mathisson's helical motions demystified". AIP Conf. Proc. AIP Conference Proceedings. 1458: 367–370. arXiv:1206.7093 . Bibcode:2012AIPC.1458..367C. doi:10.1063/1.4734436. S2CID 119306409.

Selected papers

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