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Relative velocity decomposition of a future unit timelike vector
Statement
Let be a time-oriented smooth Lorentzian four-manifold, let , let be an observer at , let be a real parameter, and let be future unit timelike, (Observers, rest spaces and the spatial projection at an event). Put
where is the spatial projection. Then:
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, with if and only if ; in particular is well defined.
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, , and
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Uniqueness. If with and , then and .
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Converse. Conversely, if and satisfy , then is future unit timelike, and ; the maps and are mutually inverse bijections between the future unit timelike vectors and the pairs with , and .
Facts & Assumptions
Given: A time-oriented smooth Lorentzian four-manifold , a point , an observer at , a real and a future unit timelike .
An observer is a vector with and ; the spatial projection is , and a future unit timelike vector is a future-directed vector with (Observers, rest spaces and the spatial projection at an event, Timelike, null, spacelike and causal vectors of a Lorentz vector space, Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model).
is linear, , , with for , the projection identity holds, and is positive definite on (The observer rest-space decomposition and the spatial projection).
If is nonzero future causal then ; if is unit timelike then is future-directed exactly when (Pairing of an observer with future causal vectors).
Proof
The vector is nonzero and future causal, so [L3] gives ; thus is well defined and belongs to because does by [L2].
Conversely let and with , and set . Then , so is unit timelike, and , so is future-directed by [L3]. Moreover and by [L2].
By the projection identity of [L2] applied to , and using , we get ; the left-hand side is because it is the square of the -norm of and is positive definite on , with equality if and only if . Since by step 1.1, gives , and holds exactly when , i.e. by [L2], which for future unit timelike means . This proves claim 1.
By the decomposition of [L2] and , we have , which is the formula of claim 2.
Suppose with and . Pairing with gives , hence . Applying and using linearity, and [L2] gives , hence . This proves claim 3.
From and step 2.1, , because is a finite real number with by step 2.1, so and . This strict bound also holds when , in which case and . This completes claim 2.
Steps 1.1-2.2 prove claims 1 and 2; step 2.3 proves claim 3; and step 1.2 together with steps 1.1-2.2 shows that the two assignments are mutually inverse on the stated sets, completing claim 4.
Depends on
Observers, rest spaces and the spatial projection at an event
The observer rest-space decomposition and the spatial projection
Pairing of an observer with future causal vectors
Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model
Timelike, null, spacelike and causal vectors of a Lorentz vector space
Dependency tree · 2 levels
Sources
- S. M. Carroll, Lecture Notes on General Relativity, arXiv:gr-qc/9712019v1 (1997), Ch. 1 'Lorentz transformations' and the Lorentz factor (printed pp. 4-6; PDF pp. 11-13) and 'four-velocity' U^mu = dx^mu/dtau with eta_mu nu U^mu U^nu = -1 (1.98)-(1.99), printed pp. 26-27 (PDF pp. 33-34)
- H. S. Reall, Part III General Relativity (Cambridge, October 12, 2022 revision), section 2.3: the 4-velocity as the unit tangent of a timelike curve, g_ab u^a u^b = -1 (2.14), printed p. 28 (PDF p. 29), and section 6.3: the observer energy E = -g_ab(p) v^a(p) P^b(p) (6.19), printed p. 64 (PDF p. 65)
- E. Gourgoulhon, 3+1 Formalism and Bases of Numerical Relativity, arXiv:gr-qc/0703035 (2007), Ch. 5, section 5.3: the orthogonal decomposition u = Gamma(n + U) of a 4-velocity with respect to an observer, with n.U = 0 and Gamma = (1 - U.U)^-1/2 (5.29)-(5.36), printed pp. 76-77