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Titlebook: General and Statistical Thermodynamics; Raza Tahir-Kheli Textbook 2020Latest edition The Editor(s) (if applicable) and The Author(s), unde

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發(fā)表于 2025-3-28 16:55:20 | 只看該作者
42#
發(fā)表于 2025-3-28 18:58:26 | 只看該作者
43#
發(fā)表于 2025-3-29 02:13:00 | 只看該作者
General and Statistical Thermodynamics978-3-030-20700-7Series ISSN 1868-4513 Series E-ISSN 1868-4521
44#
發(fā)表于 2025-3-29 04:45:03 | 只看該作者
J. Jerosch,A. Weipert,St. Hanusekmbers of particles, one might use terms like thermodynamic system; adiabatically isolating, and adiabatically enclosing, walls; adiabatic and nonadiabatic enclosures; conducting and/or diathermal walls; isothermal, isobaric, isochoric, quasistatic, reversible, and irreversible processes; state funct
45#
發(fā)表于 2025-3-29 08:43:32 | 只看該作者
Heinz U. Lemke,Kiyonari Inamura,Roland Felixhe complexity of the real systems. But the payoff of such simplicity is the ability to fully predict and understand the model system. The hope always is that such understanding will give insight into the physics of the real system of interest. Section?. refers to perfect gases.
46#
發(fā)表于 2025-3-29 13:49:03 | 只看該作者
47#
發(fā)表于 2025-3-29 16:57:30 | 只看該作者
https://doi.org/10.1007/978-1-4615-2045-0 a system, and none of it escapes, then all of it must still be there. And if there should exist a procedure to convert some of this heat energy to work, say ., then after such conversion only . of it will still be present in the system. We call this increase in the system’s internal energy the left
48#
發(fā)表于 2025-3-29 23:15:44 | 只看該作者
https://doi.org/10.1007/978-3-322-91958-8e following. Real molecules have finite size and they interact with each other. Ideal molecules are of zero size and have no interaction. Relevant description is presented in Sect.?.. In 1873 when Johannes Diderik Van der Waals presented his famous equation of state, little detail was available abou
49#
發(fā)表于 2025-3-30 02:20:06 | 只看該作者
Tree-Searching and Tree-Pruning Techniquesy of two neighboring equilibrium states is linearly related to the corresponding difference, ., in their entropy. Of course, also included in this relationship is the heat energy quasistatically added to the system and the quasistatic work, ., performed by the system when it transitions from a state
50#
發(fā)表于 2025-3-30 04:08:38 | 只看該作者
The Telephone Network as a Medium, in Sect.?.. The requirement that entropy must be maximum possible is analyzed in Sect.?.. The extremum in energy, namely that energy must be the minimum possible, is discussed in Sect.?.. The fact that the physical consequences of both these extrema are similar is noted and emphasized. Of course, a
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