consider two physical systems, Al and A2,the two systems into thermal contact with each other, thus allowing the possibility of exchange of energy between the two; this can be done by sliding in a conducting wall and removing the impervious one. The two systems are still separated by a rigid, impenetrable wall; show that the absolute value of the entropy of a given physical system in tems of the total number of microstates is S = k Lnn %3D
consider two physical systems, Al and A2,the two systems into thermal contact with each other, thus allowing the possibility of exchange of energy between the two; this can be done by sliding in a conducting wall and removing the impervious one. The two systems are still separated by a rigid, impenetrable wall; show that the absolute value of the entropy of a given physical system in tems of the total number of microstates is S = k Lnn %3D
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consider two physical systems, Al and A2,the two systems into thermal contact with each
other, thus allowing the possibility of exchange of energy between the two; this can be done
by sliding in a conducting wall and removing the impervious one. The two systems are still
separated by a rigid, impenetrable wall; show that the absolute value of the entropy of a
given physical system in tems of the total number of microstates is S = k Lnn
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