There are two masses of finite size in contact with a constant thermal reservoir. Initially, the masses are separated, with one at a higher, or hotter, temperature (Th) than the other (it is colder, at Te). The hotter mass has a heat capacity Ch, and the colder mass a heat capacity Ce. Both masses are in an adiabatic chamber. The masses are slowly brought into contact and thermal equilibrium is reached. Calculate the change in entropy of the system, and show that when Ch = Ce = C, that change is described by the expression: Th + Te 2C In 2 ThTc Is this entropy change physically reasonable?

Elements Of Electromagnetics
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ISBN:9780190698614
Author:Sadiku, Matthew N. O.
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There are two masses of finite size in contact with a constant thermal reservoir. Initially, the masses
are separated, with one at a higher, or hotter, temperature (Th) than the other (it is colder, at Te).
The hotter mass has a heat capacity C and the colder mass a heat capacity C.. Both masses are
in an adiabatic chamber. The masses are slowly brought into contact and thermal equilibrium is
reached. Calculate the change in entropy of the system, and show that when Ch = Ce = C, that
change is described by the expression:
()
Th + Tc
2C In
2, ThTc
Is this entropy change physically reasonable?
Transcribed Image Text:There are two masses of finite size in contact with a constant thermal reservoir. Initially, the masses are separated, with one at a higher, or hotter, temperature (Th) than the other (it is colder, at Te). The hotter mass has a heat capacity C and the colder mass a heat capacity C.. Both masses are in an adiabatic chamber. The masses are slowly brought into contact and thermal equilibrium is reached. Calculate the change in entropy of the system, and show that when Ch = Ce = C, that change is described by the expression: () Th + Tc 2C In 2, ThTc Is this entropy change physically reasonable?
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