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# Category: Technical

# Technical

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## (Poster) Static vs Falling: Time slicings of Schwarzschild black holes

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## Tetrad for Schwarzschild metric, in terms of e

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## Tetrad for Schwarzschild metric

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## Lorentz factor identity

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## Radial motion in the Schwarzschild metric, relative to stationary observers

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## Radial motion in the Schwarzschild metric, in terms of *e*

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## Relative speed

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Advanced content suitable for researchers

I presented this poster, “Static vs Falling: Time slicings of Schwarzschild black holes” at the GR21 conference in New York City, July 2016. You can download a PDF version. A big thank-you to those who gave feedback, especially to Jiří Podolský who encouraged me to publish it! Also the section on coordinate vectors has been updated.

The following is a natural choice of orthonormal tetrad for an observer moving radially in Schwarzschild spacetime with “energy per unit rest mass” *e*:

The components are given in Schwarzschild coordinates. (The ± signs are not independent — they must be either both +1 or both -1. Note that *e* does not distinguish between inward and outward motion. There is additional freedom to define any of these vectors as their negative.)

We normally think of *e* as invariant, where there is a presumption of freely falling / geodesic motion, but even if not we can regard it as an instantaneous value.

is the 4-velocity computed previously. The other vectors can be obtained from substituting and into the tetrad here. is determined from and the equation for *e* above, then *V* follows from inverting . This orthonormal frame is useful for determining the object’s perspective, e.g. tidal forces, visual appearances, etc.

Suppose an observer **u** moves radially with speed (3-velocity) relative to “stationary” Schwarzschild observers, where we define as inward motion. Then one natural choice of orthonormal tetrad is:

where the components are given in Schwarzschild coordinates. This may be derived as follows.

The Schwarzschild observer has 4-velocity

because the spatial coordinates are fixed, and the *t*-component follows from normalisation (Hartle §9.2).

Now the Lorentz factor for the relative speed satisfies , and together with normalisation and the assumption that the θ and φ components are zero, this yields given above.

We obtain by orthonormality: and , and again making the assumption the θ and φ components are zero. Note the negative of the *r*-component is probably an equally natural choice. Then and follow from simply normalising the coordinate vectors.

Strictly speaking this setup only applies for , because stationary timelike observers cannot exist inside a black hole event horizon! Yet remarkably the formulae can work out anyway (MTW …) . An alternate approach is local Lorentz boost described shortly.

Hartle … Also check no “twisting” etc…

A simple but useful identity is:

This follows from the definition of the Lorentz factor γ in terms of a relative speed *V* between two frames:

So

Alternatively raise both sides of the γ defining formula to the power of -2, obtaining , then multiply both sides by γ^{2} and rearrange.

Last time we derived the 4-velocity **u** of a small test body moving radially in the Schwarzschild geometry, in terms of *e*, the “energy per unit rest mass”. Another parametrisation is in terms of the 3-speed *V* relative to stationary observers. This turns out to be, in Schwarzschild coordinate expression,

To derive this, first consider the 4-velocity of stationary observers:

We know the “moving” body has 4-velocity **u** of form since the motion is radial. The Lorentz factor for the relative speed is

Evaluating and rearranging yields . Normalisation leads to , after some algebra including use of the identity . We allow also, and define this as inward motion. Carefully considering the sign, this results in the top equation. (An alternate derivation is to perform a local Lorentz boost. *Later articles will discuss this*… The Special Relativity formulae cannot be applied directly to Schwarzschild coordinates.)

Some special cases are noteworthy. For *V*=0, γ=1, and **u** reduces to **u**_{Schw}. This corresponds to . Also we can relate the parametrisation by *V* (and γ) to the parametrisation by *e* via

where the leftmost equation follows from the definition , and subsequently the rightmost equation from γ=γ(*V*). For raindrops with *e*=1, the relative speed reduces to .

We would expect the construction to fail for , as stationary timelike observers cannot exist there, and so the relative speed to them would become meaningless. But curiously, it can actually work for a faster-than-light *V*>1 “Lorentz” boost, as even the authorities MTW (§31.2, explicit acknowledgement) and Taylor & Wheeler (§B.4, implicitly *v*_{rel}>1 for *r*<2*M*) attest. Sometime, I will investigate this further…

A nice way to parametrise the 4-velocity **u** of a small test body moving radially within Schwarzschild spacetime is by the “energy per unit rest mass” *e*:

For the “±” term, choose the sign based on whether the motion is inwards or outwards. All components are given in Schwarzschild coordinates . The result was derived as follows. In geometric units, the metric is:

By definition , where is the Killing vector corresponding to the independence of the metric from *t*, and has components (Hartle §9.3). For geodesic (freefalling) motion *e* is invariant, however even for accelerated motion *e* is well-defined instantaneously and makes a useful parametrisation.

We want to find say. Rearranging the defining equation for *e* gives . Radial motion means , so the normalised condition yields the remaining component . The resulting formula is valid for all , and for *e*=1 the 4-velocity describes “raindrops” as expected.

Suppose two observers at the same place and time (that is, “event”) move with 4-velocities **u** and **v** respectively, then they measure their relative speed as follows. The Lorentz factor is simply

(The dot is not the Euclidean dot product, but uses the metric: where the indices and are summed over by the Einstein summation convention.) The proof is based on the axiom that some local inertial frame exists, although interestingly one does not need to explicitly construct it.

The relative 3-speed *V*, may then be recovered via:

See for instance Carroll (end of §2.5) who terms it “ordinary three-velocity”. Other sources express the first formula more indirectly, in terms of the energy and momentum measured by an observer : where is the 4-momentum of another observer/object, and combine this with (MTW Exercise 2.5 in §2.8 term it “ordinary velocity”, or Hartle §5.6, and Example 9.1 in §9.3).