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Now that the enthalpy and entropy of state four was known all the other properties could be obtained through RefProp. Next state two’s properties were determined through a similar analysis as state four. Since the heat input added to the boiler was known and the ideal assumption implies that the pressure at state two would be equal to the pressure at state three all the properties at state two were able to be calculated. In order to calculate the enthalpy at state two the following equations were used. (2.6) (2.7) Now that state two’s enthalpy and pressure were known the remaining properties could be obtained using RefProp. State one’s properties are the only ones left to be determined now. State one’s properties could be calculated in two different ways. The first way to do this was using the ideal assumption again. The heat rejection happens at a constant pressure therefore the pressure at state one is equivalent to the pressure at state four. The pumping happens at constant entropy which means that state one’s properties can be defined by the two independent properties of entropy and pressure. The problem that arises by using this assumption is that sometimes the quality at state one based solely on the entropy and pressure was not always zero. This is a problem because the fluid should be in liquid form when it exits the condenser at state one. The second way to determine state one is similar to the process used to define state three. The pressure in state one is assumed to be equivalent to the 28PDF Image | NESTER, RYAN TIMOTHY. Organic Rankine Cycles: A Comparative Study and Analysis of Multiple Applications.
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