Di Liberto, Francesco and Pastore, Raffaele and Peruggi, Fulvio (2011) Dissipated energy and Entropy Production for an Unconventional Heat Engine: The Stepwise “Circular Cycle”.

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Item Type:  Article 

Uncontrolled Keywords:  Entropy production; Thermodynamics; Recovery; Thermal analysis 
Date Deposited:  24 Feb 2011 16:34 
Last Modified:  30 Apr 2014 19:43 
URI:  http://www.fedoa.unina.it/id/eprint/7896 
Abstract
When some entropy is transferred, by means of a reversible engine, from a hot heat source to a colder one, we have the maximum of efficiency, i.e. we obtain the maximum available work. Similarly the reversible heat pumps transfer entropy from a cold heat source to a hotter one with the minimum expense of energy. On the contrary if we are faced with non reversible devices there is some Lost Work for heat engines, and some Extra Work for heat pumps. These quantities are both related to the Entropy production. The Lost Work, i.e. WLost = WRev  WIrrev, is also called ‘degraded energy’ or ‘Energy unavailable to do work’. The Extra Work, i.e. WExtra = WIrrev  WRev, is the excess of work performed on the system in the irreversible process with respect to the reversible one (or the excess of heat given to the hotter source in the irreversible process). In this paper, which follows two previous ones on the Lost Work [Phil. Mag. 87, 569 (2007), Phil. Mag. 88 41774187 (2008)] both quantities are analyzed in deep and are evaluated for a process with complexity, i.e. the stepwise Circular Cycle which is similar to the stepwise Carnot cycle [Physica A314, 331 (2002)]. The stepwise Circular Cycle is a cycle performed by means of N small weights dw which are first added and then removed from the piston of the vessel containing the gas or viceversa. The work performed by the gas can be found as increase of the potential energy of the dw’s. We identify each single dw and thus evaluate its rising i.e. its increase in potential energy. In such a way we find how the energy output of the cycle is distributed among the dw’s. The size of the dw’s affects the Entropy production and therefore the Lost and Extra work. The rising distribution depends on the removing process we choose.
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