An adiabatic thermalization between $n$ bodies is an irreversible process, leading to a rise in the total entropy of the bodies and yields a final common temperature $T_F$. We express the Clausius formula that computes the entropy change between the initial non-equilibrium state and the final equilibrium state, using another equilibrium state of the $n$ bodies for the given initial entropy, that corresponds to a temperature $T_f$. The second law inequality follows from the fact $T_f < T_F$, under the assumption of positive heat capacities of the bodies. We derive this inequality for the discrete case of $n$ bodies as well as the continuum case of an unequally heated rod. As an example, we illustrate our results for the case of temperature-i...
10.1073/pnas.1411728112Proceedings of the National Academy of Sciences of the United States of Ameri...
We show that both positive and negative absolute temperatures and monotonically increasing and decr...
In 1854 Clausius proved the famous theorem that bears his name by assuming the second "law" of therm...
Recently, there have appeared interesting correctives or challenges [Entropy 1999, 1, 111-147] to th...
The example of macroscopic thermodynamical system violating the Clausius inequality is presented
In a previous work (M. Campisi. Stud. Hist. Phil. M. P. 36 (2005) 275-290) we have addressed the mec...
In a previous work (M. Campisi. Stud. Hist. Phil. M. P. 36 (2005) 275-290) we have addressed the mec...
In a previous work (M. Campisi. Stud. Hist. Phil. M. P. 36 (2005) 275-290) we have addressed the mec...
Considering intrinsic characteristics of the system exclusively, both statistical and information th...
Total energy conservation resolves all sources of heat. First Law of thermodynamics does not repres...
The second law of thermodynamics is often expressed as the fact that the entropy of an isolated syst...
peer reviewedThe amount of work that is needed to change the state of a system in contact with a he...
We show that both positive and negative absolute temperatures and monotonically increasing and decre...
At its origins, thermodynamics was the study of heat and engines. Carnot transformed it into a scien...
We show that both positive and negative absolute temperatures and monotonically increasing and decre...
10.1073/pnas.1411728112Proceedings of the National Academy of Sciences of the United States of Ameri...
We show that both positive and negative absolute temperatures and monotonically increasing and decr...
In 1854 Clausius proved the famous theorem that bears his name by assuming the second "law" of therm...
Recently, there have appeared interesting correctives or challenges [Entropy 1999, 1, 111-147] to th...
The example of macroscopic thermodynamical system violating the Clausius inequality is presented
In a previous work (M. Campisi. Stud. Hist. Phil. M. P. 36 (2005) 275-290) we have addressed the mec...
In a previous work (M. Campisi. Stud. Hist. Phil. M. P. 36 (2005) 275-290) we have addressed the mec...
In a previous work (M. Campisi. Stud. Hist. Phil. M. P. 36 (2005) 275-290) we have addressed the mec...
Considering intrinsic characteristics of the system exclusively, both statistical and information th...
Total energy conservation resolves all sources of heat. First Law of thermodynamics does not repres...
The second law of thermodynamics is often expressed as the fact that the entropy of an isolated syst...
peer reviewedThe amount of work that is needed to change the state of a system in contact with a he...
We show that both positive and negative absolute temperatures and monotonically increasing and decre...
At its origins, thermodynamics was the study of heat and engines. Carnot transformed it into a scien...
We show that both positive and negative absolute temperatures and monotonically increasing and decre...
10.1073/pnas.1411728112Proceedings of the National Academy of Sciences of the United States of Ameri...
We show that both positive and negative absolute temperatures and monotonically increasing and decr...
In 1854 Clausius proved the famous theorem that bears his name by assuming the second "law" of therm...