Thermodynamics SECOND LAW OF THERMODYNAMICSPump efficiency, , relates the work required by an ideal pump to the actual work required byh pthe pump; it relates the minimum amount of work theoretically possible to the actual workrequired by the pump. However, the work required by a pump is normally only an intermediateform of energy. Normally a motor or turbine is used to run the pump. Pump efficiency doesnot account for losses in this motor or turbine. An additional efficiency factor, motor efficiency, is defined as the ratio of the actual work required by the pump to the electrical energy inputh mto the pump motor, when both are expressed in the same units.h mWp, actualWm, inCwhere:= motor efficiency (no units)h mWp, actual= actual work required by the pump (ft-lbf)Wm, in= electrical energy input to the pump motor (kw-hr)C = conversion factor = 2.655 x 106 ft-lbf/kw-hrLike pump efficiency , motor efficiency is always less than 1.0 or 100% for an actualh ph mpump motor. The combination of pump efficiency and motor efficiency relates the idealh ph mpump to the electrical energy input to the pump motor.(1-35)h mh pWp, idealWm, inCwhere:= motor efficiency (no units)h m= pump efficiency (no units)h pWp, ideal= ideal work required by the pump (ft-lbf)Wm, in= electrical energy input to the pump motor (kw-hr)C = conversion factor = 2.655 x 106 ft-lbf/kw-hrA heat exchanger is designed to transfer heat between two working fluids. There are several heatexchangers used in power plant steam cycles. In the steam generator or boiler, the heat source(e.g., reactor coolant) is used to heat and vaporize the feedwater. In the condenser, the steamexhausting from the turbine is condensed before being returned to the steam generator. Inaddition to these two major heat exchangers, numerous smaller heat exchangers are usedthroughout the steam cycle. Two primary factors determine the rate of heat transfer and thetemperature difference between the two fluids passing through the heat exchanger.Rev. 0 Page 83 HT-01
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