
Both are important differences. But many results from the non-relativistic theory will remain formally valid.
Thus for instance in the relativistic case we still have
with just like (33 We recall the discussion – in Section 4.2 – of the important role played by
in ensuring symmetric
hyperbolicity of the field equations: Symmetric hyperbolicity was due to the concavity of
in the
privileged frame moving with the four-velocity
. Now we see from (72
) that – for the
non-degenerate gas – we have
so that the privileged frame is the local rest frame of the gas.
This is quite satisfactory, since the rest frame is naturally privileged. [There remains the question of why
the rest frame is not the privileged one for a degenerate gas. This point is open and invites
investigation.]
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