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Titlebook: Nonlinear Nonequilibrium Thermodynamics II; Advanced Theory Rouslan L. Stratonovich Book 1994 Springer-Verlag Berlin Heidelberg 1994 Nichtg

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11#
發(fā)表于 2025-3-23 13:27:07 | 只看該作者
,The Kirchhoff’s Form of Fluctuation-Dissipation Relations,ave motion described by linear equations in the presence of bodies that interact, linearly or nonlinearly, with the waves. These relations are a generalization of the well-known Kirchhoff’s law to the case of any degree of coherence of waves, and also to the case of a possible nonlinear interaction
12#
發(fā)表于 2025-3-23 15:58:37 | 只看該作者
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發(fā)表于 2025-3-23 21:32:30 | 只看該作者
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發(fā)表于 2025-3-23 23:44:01 | 只看該作者
15#
發(fā)表于 2025-3-24 04:39:55 | 只看該作者
Rouslan L. Stratonovichost out of each Caldwell object by using the most suitable eWhen Mike Inglis, who consults for Springer, ? rst asked me to write a Caldwell book in their “and How to Observe Them” series I admit I did need some time to think the suggestion over. I am a fan of Patrick’s Caldwell catalog as are most o
16#
發(fā)表于 2025-3-24 09:20:39 | 只看該作者
17#
發(fā)表于 2025-3-24 12:22:27 | 只看該作者
18#
發(fā)表于 2025-3-24 15:33:10 | 只看該作者
time to think the suggestion over. I am a fan of Patrick’s Caldwell catalog as are most of the amateur astronomers I know, but could a new book be justi? ed when the massive, compreh- sive, and wrist-spraining Caldwell tome by Stephen O’Meara covers the subject fully anyway? That other book was res
19#
發(fā)表于 2025-3-24 20:43:57 | 只看該作者
Nonequilibrium Thermodynamics of Open Systems,open systems the important fundamental principle of time-reversal invariance does not exist. Therefore, in the case of open systems there are fewer FDRs than before, and they are not so effective. There is only one linear relation, one quadratic FDR and one cubic FDR.
20#
發(fā)表于 2025-3-25 00:57:37 | 只看該作者
Method of Projection in Space of Phase Space Distributions and Irreversible Processes,kov nature of the macroprocess in question. It is useful then to apply a projection operator defined in the space of phase space distributions. Formally, irreversibility appears as a consequence of a combination of actions of the projection operator and the time-evolution operator.
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