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Curves in Figure-12A and Figure-12B can be categorized into two groups. The first group includes cases which provide more than enough heat energy for the GM to generate maximum allowed power output of 50kW. For these cases, the excess heat energy is dissipated into cooling water which causes the net GM efficiency to drop (even if the net power output increases) due to the increased amount of heat lost into the cooling water. The second group contains the cases of which the maximum gross outputs are less than 50kW. The gross output of these cases are not proportional to the input heat energy, due to the limited (designed) heat transfer area of the heat exchanger, of which the effectiveness reduces while flow rate increases over certain flow rates. For these cases the gross output power are increasing at slower rate for higher flow rate but the net efficiency increases with a slower rate or even may decrease with higher flow rate. Similar trends are seen with other cold water flow rate plots and the same discussion is valid for Figures 13A & 13B as well as Figure 14A & 14B. Figure-13A: Screw expander and GM net power output for different hot water flow rates and temperatures at cold water condition of 160gpm @ 50oF 52PDF Image | Optimizing Heat Recovery Systems for Power Generation in Rural AK
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