HIGHLIGHTS
SUMMARY
Quantum mechanics and general relativity both require the notion of space and time, whereas classical thermodynamics has so far only addressed space as a hidden variable, for example, as the "volume" in the ideal gas equation, and has only implicit time dependence, e_g, in the "initial" and "final" states. Expectations range from a possible description of relations between forces and temperature as found, e_g, in the Unruh temperature, to special relativity and perhaps further unexpected terms and equations. It relates, e_g, to heat and work or Carnot cycles and originates from the age of . . .
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