Gyarmati's Variational Principle of Dissipative Processes
نویسنده
چکیده
Like mechanics and electrodynamics, the fundamental laws of the thermodynamics of dissipative processes can be compressed into a variational principle. This variational principle both in its differential (local) and in integral (global) forms was formulated by Gyarmati helped by the present author in 1965. This principle was applied to several fields of irreversible processes: first of all, his colleagues (Verhás [1], Böröcz [2], Farkas [3,4], Sándor [5], Vincze [6–8], Stark [9,10]); but also many others (Singh [11,12], Bhattacharya [13,14], Dickel [15,16] etc.). Consistent application of both the local and the global forms of Gyarmati’s principle provides all the advantages throughout explicating the theory of irreversible thermodynamics that are provided in the study of mechanics and electrodynamics by the corresponding classical variational principles, e.g., Gauss’ differential principle of least constraint, or Hamilton’s integral principle. THE GOVERNING PRINCIPLE OF DISSIPATIVE PROCESSES (GPDP) Gyarmati’s principle is based on the fact that the generalization of the dissipation functions — that were introduced by Rayleigh and Onsager for special cases — always exist locally in continua [17–22]. In linear theory these functions are defined as:
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ورودعنوان ژورنال:
- Entropy
دوره 16 شماره
صفحات -
تاریخ انتشار 2014