A Treatise of Heat and Energy by Lin-Shu Wang

A Treatise of Heat and Energy by Lin-Shu Wang

Author:Lin-Shu Wang
Language: eng
Format: epub
ISBN: 9783030057466
Publisher: Springer International Publishing


6.2 Quasi-static Processes and the Classical (Caratheodory) Formalism

Carathéodory [3] set out to develop an alternative formulation to the definition of entropy , (62A), in Chap. 5, without using the reversible thermal machines. He began by noting the application of the first law, , to an adiabatic composite system (which consists of subsystems, e.g., two subsystems “1” and “2”) separated diathermanously undergoing quasi-static adiabatic processes

Because of being diathermanously related, the two subsystems are at the same temperature.

By “quasi-static” he meant, “A process that occurs so slowly that the difference between the work performed externally and the preceding limit, pdV, is smaller than the uncertainty of our measurements” [3:238]. A quasi-static process is an infinitely slow process.

On the same page, however, he added, “a quasistatic adiabatic process can be regarded as a series of [infinitely dense succession of] equilibrium states” [3:238]. Callen [5:96] also defined quasi-static processes to be “in terms of a dense succession of equilibrium states.” I make the interpretation here that both Carathéodory and Callen equated infinitely dense processes with infinitely slow processes as synonymous terms. In the following, a restated version is used for discussion in this chapter as the definition of quasi-static process (quasi-equilibrium process) set:The set consists of a subset-series of infinitely dense succession of equilibrium states and the corresponding subsets of all spontaneous transient states between each pairs of equilibrium states in the series.



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