Abstract

Using a van der Waals gas as the working substance the so called Curzon and Ahlborn-Novikov engine is studied. It is shown that some previous results found in the literature of finite time thermodynamics can be written in a more general form, means of this gas and by taking a non linear heat transfer law.

Highlights

  • In classical equilibrium thermodynamics the efficiency of a reversible thermal engine operating between two reservoirs, at temperatures T1w > T2w, is known to be: ηC= 1 − T2w T1w (1.1)Entropy 2005, 7[1]In this description the temperatures of the working substance along the isothermal branches, T1w, i = 1,2, are assumed to be the same as the corresponding reservoirs; as a consequence the processes associated with the heat transfer between the engine and the reservoirs are ignored

  • By taking into account the time explicitly for all the branches of the cycle in terms of thermodynamic properties, and with the heat transfer Newton's law, Gutkowics-Krusin et al.[31] have shown that the Curzon and Ahlborn-Novikov efficiency ηCAN is an upper bound for the efficiency as a function of both the ratio β and the ratio of the maximum and the minimum volume spanned by the cycle, through the quantity ln

  • Ladino-Luna[33] has shown that ecological function has the same form in [14] if it is taken as working substance a van der Waals gas as well as it is using an ideal gas as the working substance, in the case of Newton heat transfer law, by taking the change V → V − b, where b is a constant that depends on the system

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Summary

Introduction

By taking into account the time explicitly for all the branches of the cycle in terms of thermodynamic properties, and with the heat transfer Newton's law, Gutkowics-Krusin et al.[31] have shown that the Curzon and Ahlborn-Novikov efficiency ηCAN is an upper bound for the efficiency as a function of both the ratio β and the ratio of the maximum and the minimum volume spanned by the cycle, through the quantity ln Ladino-Luna[33] has shown that ecological function has the same form in [14] if it is taken as working substance a van der Waals gas as well as it is using an ideal gas as the working substance, in the case of Newton heat transfer law, by taking the change V → V − b , where b is a constant that depends on the system.

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