I Why is Number-Flux Four-Vector Frame-Independent?

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The discussion centers on the frame independence of the number-flux four-vector, defined as N = nU, where n is number density and U is four-velocity. It clarifies that all four-vectors are inherently frame independent due to their geometric nature. The conversation emphasizes that while the components of the four-velocity and number density are frame dependent, their combination in the form of the number-flux four-vector remains invariant across different frames. This invariance is crucial for understanding how particle flux behaves under transformations in relativity. The discussion highlights the importance of recognizing the meaningful representation of these quantities in both local rest frames and broader relativistic contexts.
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Recently I started studying 《A First Course in General Relativity》 and I came across a question in my book:
##\vec N =n\vec U##where n is number density,U is four-velocity,N is number-flux four-vector .The following sentence confused me:
In Galilean physics,number density was a scalar,the same in all frames(no Lorentz contraction),while flux was quite another thing:a three-vector that was frame dependent,since the velocities of particles are a frame-dependent notion.Our relativistic approach has unified these two notions into a single,frame-independent four-vector...
I wonder Why the number-flux four-vector is frame-independent?
 
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All four-vectos are frame independent

You should read page 88 (in the second edition) where it is explained what 'frame independent' means in this case
 
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GR191511 said:
I wonder Why the number-flux four-vector is frame-independent?
Because it's a four vector. They're frame independent by construction.

I think what you need to do is convince yourself that ##nU^a## actually represents something meaningful, and that it represents something meaningful whether ##U^a## is parallel to your frame's timelike axis or not. The usual way to go about it is to imagine a very large number of particles each with velocity ##U^a##. Then convince yourself that the number of particles crossing an infinitesimal plane depends on the number density ##n## and the velocity field ##U^a##, then convince yourself that the transformation properties of ##U^a## supply the right factors of ##\gamma## so that the transformed flux density behaves as you expect.
 
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The components of the 4-velocity are still frame dependent even if the 4-velocity itself is an invariant geometric object. This means that also the number density itself is frame dependent in relativity (##n## is the number density in the rest frame and is a scalar) just as the flux, which is number density times velocity just as in Galilean spacetime.
 
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Yes, and that's why one defines (!) such medium-related "intrinsic" quantities in the local rest frame(s) of the fluid and thus becoming a scalar. That holds also for thermodynamic quantities like temperature or chemical potential.
 
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Moderator's note: Spin-off from another thread due to topic change. In the second link referenced, there is a claim about a physical interpretation of frame field. Consider a family of observers whose worldlines fill a region of spacetime. Each of them carries a clock and a set of mutually orthogonal rulers. Each observer points in the (timelike) direction defined by its worldline's tangent at any given event along it. What about the rulers each of them carries ? My interpretation: each...

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