Calculating Efficiency of Heat Engine with Steam in Saturation Dome

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The discussion focuses on calculating the efficiency of a heat engine operating with steam in the saturation dome, specifically using pressures of 1 MPa for heat addition and 0.5 MPa for heat rejection. The highest possible efficiency can be determined using the Carnot efficiency formula, η_max = 1 - T_c/T_h, where T_h and T_c are the temperatures corresponding to the pressures. The temperatures are approximately 180ºC (353K) for the high pressure and 150ºC (323K) for the low pressure. There is some confusion regarding the use of the coefficient of performance (COP) in the context of a heat engine, as it is typically associated with heat pumps rather than engines. Understanding these principles is crucial for accurately calculating the engine's efficiency.
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Q. A heat engine cycle is executed with steam in the saturation dome. The pressure of steam is 1 MPa during heat addition and 0.5 MPa during heat rejection. THe highest possible efficiency of the heat engine is.

How to calculate heat efficiency?

W = QH / COP,hp

and

COP = 1 / ( TH /TL - 1 )

Pl. note COP- denotes the coefficient of performance of the heat engine.

Any ideas on how to proceed?

Thanks, a lot!
 
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Naeem said:
Q. A heat engine cycle is executed with steam in the saturation dome. The pressure of steam is 1 MPa during heat addition and 0.5 MPa during heat rejection. THe highest possible efficiency of the heat engine is.

How to calculate heat efficiency?

W = QH / COP,hp

and

COP = 1 / ( TH /TL - 1 )

Pl. note COP- denotes the coefficient of performance of the heat engine.

Any ideas on how to proceed?

Thanks, a lot!

It seems to me that the engine is working with a Rankine Cycle. Anyway, during the change of state the pressure and temperature remains constant. If you have the pressure 1MPa then you have the temperature of saturation of water (T_h=180ºC=353K) and the pressure 0.5 Mpa gives you T_c=150ºC=323K aproximately (verify the data in a table of water).

This means the engine, maybe an steam machine, is vaporizing water in the boiler at temperature T_h which may be the hot focus (maybe it is not totally true in a Rankine cycle because the bolier superheats the vapor), and is condensing the vapor at temperature T_c in the condenser. The second principle of the thermodynamics states than the maximum efficiency is reached by means of a Carnot engine working between the two extreme temperatures:

\eta_{max}=\frac{W}{Q_h}=1-T_c/T_h

I don't really understand why you used the COP when we are talking about an engine.
 
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