Four Velocity Sign of Time: \dot t>0?

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SUMMARY

The discussion centers on the concept of four-velocity in the context of light-like paths in spacetime. It is established that four-velocity is not defined for null paths, as noted by @Sagittarius A-Star. However, four vectors tangent to null curves, such as four momentum, can be defined. For massive particles, the proper time parameter, denoted as ##\tau##, allows for a normalized four-velocity where ##u_{\mu} u^{\mu}=c^2##, while massless particles can utilize any affine parameter, maintaining the condition ##\dot{x}^{\mu} \dot{x}_{\mu}=0## for light-like worldlines. In both scenarios, it is conventional to set ##\dot{t}>0## to indicate motion into the future.

PREREQUISITES
  • Understanding of four-velocity and its definitions in relativity
  • Familiarity with light-like and time-like worldlines
  • Knowledge of proper time and affine parameters
  • Basic concepts of spacetime and global distinctions between past and future
NEXT STEPS
  • Study the properties of four momentum in the context of null paths
  • Explore the implications of choosing different affine parameters for massless particles
  • Investigate the mathematical formulation of time-like and light-like worldlines
  • Learn about the normalization conditions for four-velocity in general relativity
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The discussion is beneficial for physicists, particularly those specializing in general relativity, theoretical physicists exploring spacetime concepts, and students seeking to deepen their understanding of four-velocity and its applications in relativistic physics.

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Is it generally the case even with light like paths that ##\dot t>0##?
Is it generally the case even with light like paths that ##\dot t>0##?
 
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A four velocity is not defined for a light like path.
 
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Up to you, really. It is true that all future-pointing vectors will have the same sign in their time component, assuming your time coordinate is reasonably named and the spacetime has a global distinction between past and future. But there's nothing to stop you having your time coordinate increase towards the past, in which case all future-pointing four vectors would have negative time components.

As @Sagittarius A-Star points out, four velocity is not defined for null paths. However, you can define other four vectors tangent to null curves, such as the four momentum.
 
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It's convenient to have the world-line parameter defined such that ##\dot{t}>0##. For massive particles you have time-like worldlines, and you can choose the proper time, ##\tau## as a natural world-line parameter. Then the four-velocity is "normalized": ##u_{\mu} u^{\mu}=c^2##.

For massless particles ("naive photons") of course you cannot choose proper time, because it's not defined but you can choose any affine parameter you like. Then you have ##\dot{x}^{\mu} \dot{x}_{\mu}=0##, i.e., light-like worldlines.

In both cases it is natural to choose ##\dot{t}>0##, where ##t## is the time-like coordinate since then with increasing world-line parameter you describe a motion into the future.
 
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