DrGreg
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I'm assuming that your first mention of I should have been I', which I have corrected in the quote above.bernhard.rothenstein said:Let generalize the problem. Consider that a clock K' is located at the origin O' of its rest frame I'. It measures a time interval dt(0), has a mass m(0) an energy E(0), a temperature T(0) and an extension dx(0) in the direction of the x' axis. Are all of them REST, PROPER or INVARIANT physical quanties?
Measured from I they are dt, m, T and dx. Are they RELATIVISTIC physical quantities or there are better names?
I can't comment on temperature, as that's not a subject I've studied under relativity.
Assuming we are measuring an object that is stationary relative to the I' frame, in Special (not General) Relativity:
- the relativistic mass relative to I' is the same as the rest/proper/invariant mass (all 3 mean the same)
- the energy relative to I' is the same as "rest-energy" or "rest-mass-energy"
- a time interval dt' is the same as proper time d\tau, provided we are talking about a single point in space (stationary relative to I')
- a distance interval dx' is the same as proper length or rest length
In the I frame, that same object is not stationary and so
- the relativistic mass relative to I is not rest mass
- the energy relative to I is not "rest-energy"
- a time interval dt is "coordinate time"
- a distance interval dx is "coordinate distance"
In general, coordinate measurements depend on a frame's synchronisation convention, whereas proper or invariant measurements do not.
In general relativity it gets more complicated.