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Effects of mass transfer laws on finite time exergy

机译:传质定律对有限时间火用力的影响

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The problem of the maximal work that can be extracted from a system consisting of one infinite chemical potential reservoir and one subsystem is investigated in this paper. Finite time exergy is derived for the fixed duration of the process by applying optimal control theory. Effects of mass transfer laws on the finite time exergy and the corresponding optimal mass transfer processes are analysed. The optimal thermodynamic processes for the finite time exergy include two categories: one is that the chemical potential of the subsystem is a constant and the chemical potential difference between the reservoir and the subsystem is also a constant during the mass transfer process, and the other is that the chemical potential of the subsystem switches between two optimal values during the mass transfer process. Mass transfer laws have significant effects on the optimal thermodynamic process for the finite time exergy, and the necessary and sufficient condition to determine the optimal thermodynamic process is also given. The results show that the optimal thermodynamic processes with mass transfer laws [g∝Δ(μ)] and [g∝Δ(c)], where Δμ is the chemical potential difference and Ac is the concentration difference, belong to the first category, while the optimal thermodynamic processes with mass transfer laws g∝[(Δμ) + (Δμ)~n, where n is an odd number and equal to or larger than 9, belong to the second category. The finite time exergy tends to the classical thermodynamic exergy when the duration tends to infinite long. The finite time exergy is a more realistic, stronger limit compared to the classical thermodynamic exergy.
机译:本文研究了从一个无限化学势储层和一个子系统组成的系统中可以提取的最大功问题。通过应用最佳控制理论,可以在过程的固定时间内得出有限的时间(火用)。分析了传质定律对有限时间火用的影响以及相应的最佳传质过程。有限时间火用的最佳热力学过程包括两类:一是在传质过程中子系统的化学势为常数,储层与子系统之间的化学势差也为常数。在传质过程中子系统的化学势在两个最佳值之间切换。传质定律对有限时间火用的最佳热力学过程有重大影响,并且给出了确定最佳热力学过程的充要条件。结果表明,具有传质律[g∝Δ(μ)]和[g∝Δ(c)]的最佳热力学过程属于第一类,其中Δμ是化学势差,Ac是浓度差。而具有传质律g∝ [(Δμ)+(Δμ)〜n,其中n为奇数且等于或大于9的最优热力学过程属于第二类。当持续时间趋于无穷长时,有限时间的(火用)趋向于经典的热力学(火力)。与经典的热力学能动相比,有限时间能动是一个更现实,更强的限制。

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