Exact(3)
The work and heat interactions, the exergy losses and the efficiencies of various components based on both energy and exergy concepts are evaluated.
For sake of generality, work and heat interactions are considered occurring either successively or simultaneously, and both result from generalized available energy of a simple system as defined by Gyftopoulos and Beretta[1].
This formulation would be suitable to evaluate either the net useful work or the net useful heat of a system being both the outcome of available energy, considering the role of pressure other than temperature, in the evaluation of work and heat interactions in combination with a reservoir as defined in the study of Gyftopoulos and Beretta[1].
Similar(57)
Total heat interaction over the whole Carnot cycle (J).
Through the integrated approach, the heat interaction and the heat flow are simulated and analysis together.
that represents the equivalence with the amount of heat interaction only in the isovolumic process between two different temperatures.
Annuluses 1 and 2 in Fig. 3 represent heat interaction boundaries of two independent loops: brine and working fluid.
where QR is the minimum heat interaction with the thermal reservoir and W R is the minimum work interaction with the mechanical reservoir.
With different wording, 'extended physical exergy' can be translated into 'exergy of exergy' that makes becoming work interaction equivalent to and interconvertible with heat interaction and vice versa.
that is valid if and only if entropy remains constant but, on the other side, it should change due to heat interaction occurring alongside the isothermal process.
Thus, thermal entropy variation related to heat interaction is null depending on a compensation effect due to the combination of either temperature and pressure variation.
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