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Existence of an inertial frame whose time axis is a prescribed future timelike direction
Statement
Let be the oriented time-oriented affine Minkowski space, let be a future timelike displacement and put and . Then:
(i) and is future timelike, so is a future unit timelike vector.
(ii) For every event there is an inertial frame of the model with .
(iii) For the inertial chart of any such frame one has for every real ; in particular and . Consequently, for any two events with , the chart of such a frame represents the displacement by the coordinate vector : the spatial coordinates of and agree and their time coordinates differ by .
Facts & Assumptions
Given: The oriented time-oriented affine Minkowski space and a future timelike displacement , with and .
Inertial frames and charts: for every event and every -orthonormal ordered basis of with future first vector and positive orientation, is an inertial frame; its chart is with the frame's linear isomorphism, and every vector has unique coordinates , (Inertial frames and inertial charts of the affine Minkowski model, Existence of future-oriented inertial frames at every event).
Cone coordinates: in an inertial frame with first vector in one has and , and ; the restriction of to is positive definite, is orthonormal for it, and for (The timelike set has exactly two convex components, described in orthonormal coordinates, Time orientation, future and past timelike/null/causal vectors, and the closed cones, The Euclidean spatial structure and cross product of an inertial frame).
The passive boost is defined for every parameter with (The passive Lorentz boost with parameter beta); it is a proper orthochronous Lorentz map with inverse (The passive boost is a proper orthochronous Lorentz map with inverse B(-beta), Linear and affine Lorentz maps, and the Lorentz group); and if is future timelike with and coordinates , then the parameter satisfies and , where is the first vector of the frame used for the coordinates (The passive boost is a proper orthochronous Lorentz map with inverse B(-beta) (iv)).
Lorentz maps preserve the metric and the orientation class: for a linear Lorentz map one has for all ; the composition and the inverse of Lorentz maps are Lorentz maps, and the proper orthochronous ones form a group; if is proper, then the oriented volume form of The oriented volume form epsilon and the permutation symbols of an inertial frame is preserved, ; and takes the value on every positively oriented -orthonormal basis, so a tuple of four vectors with -value is positively oriented (Lorentz maps are isomorphisms of determinant ±1 that preserve causal character and permute the cones; the Lorentz sets are groups, The oriented volume form is independent of the positively oriented inertial frame).
Square roots and monotonicity: every real has a unique with (Square roots exist: a unique with ; the positives are ); for one has (Squaring is monotone on the nonnegatives).
Order arithmetic of : multiplication of an inequality by a positive real preserves it, and a product of positives is positive (Sign rules for products and monotonicity of multiplication); a constant may be added to both sides and inequalities may be added (Order is preserved by adding a constant and by adding inequalities); and the order is trichotomous and transitive, with (Ordered field).
Proof
By bilinearity of and one has , so is timelike and ; moreover is nonzero because it is timelike, so is nonzero.
Fix an event and an inertial frame with chart , and write in its coordinates; since is timelike, [F2] puts it in or , and since with and its first coordinate satisfies , so lies in and is future timelike; in particular .
From we get ; setting (the coordinate column, identified with the vector of ) one has , hence by strict monotonicity of squaring on the nonnegatives and ; thus the passive boost is defined.
By [F3] (iv), applied to the future timelike unit vector with coordinates , the boost satisfies ; and is proper orthochronous with inverse .
Define and for ; then for all , so because a Lorentz map preserves , and the ordered basis is -orthonormal with future first vector ; it is positively oriented because is proper and preserves the oriented volume form, so for the positively oriented basis , whence the basis is positively oriented. Therefore is an inertial frame with , which is (ii).
For the chart of any inertial frame with one has and , so for every real , since is linear; in particular and , which is (iii).
Consequently, for events with , linearity of gives , so the spatial coordinates of and agree and their time coordinates differ by ; together with steps 1.1, 2.1, 5.1 and 6.1 this proves (i), (ii) and (iii).
Depends on
Oriented time-oriented affine Minkowski space (the spacetime primitives)
Lorentz forms of inertia (3,1,0) on a 4-dimensional real vector space
Timelike, null, spacelike and causal vectors of a Lorentz vector space
Time orientation, future and past timelike/null/causal vectors, and the closed cones
The timelike set has exactly two convex components, described in orthonormal coordinates
Inertial frames and inertial charts of the affine Minkowski model
Existence of future-oriented inertial frames at every event
The passive Lorentz boost with parameter beta
The passive boost is a proper orthochronous Lorentz map with inverse B(-beta)
Lorentz maps are isomorphisms of determinant ±1 that preserve causal character and permute the cones; the Lorentz sets are groups
Linear and affine Lorentz maps, and the Lorentz group
The Euclidean spatial structure and cross product of an inertial frame
The oriented volume form epsilon and the permutation symbols of an inertial frame
The oriented volume form is independent of the positively oriented inertial frame
Square roots exist: a unique with ; the positives are
Squaring is monotone on the nonnegatives
Sign rules for products and monotonicity of multiplication
Order is preserved by adding a constant and by adding inequalities
Ordered field
Dependency tree · 2 levels
Sources
- B. Crowell, Special Relativity, revision 2020-12-10 (author-published undergraduate textbook): sections 1.3.3 'The gamma factor' pp. 25-27 and 1.5 pp. 36-37; signature (+---) converted to (-+++) and c = 1 formulas converted to x^0 = c t
- S. M. Carroll, Lecture Notes on General Relativity, arXiv:gr-qc/9712019v1 (1997), Chapter 3 pp. 68-73 (proper-time functional, geodesic variation, the maximality remark and its 'locally' caveat, the twin remark)
- H. S. Reall, Mathematical Tripos Part III General Relativity (Cambridge, October 12, 2022), sections 2.1-2.3 pp. 25-30 (inertial frames and their bases; straight lines in inertial frames); Internet Archive copy of the original https://www.damtp.cam.ac.uk/user/hsr1000/part3_gr_lectures.pdf