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Figure 5‐7 shows the change in the distribution of entropy generation with an increasing system high pressure side pressure. Due to the dramatic decrease in entropy generation in the gas heater, the distribution of entropy generation in the gas heater decreases, while it increases in other system components. Figure 5‐7 Distribution of entropy generation vs. system high pressure side pressure Figure 5‐8 and Figure 5‐9 show the exergy destruction and the entropy generation in different system components against an increasing heat source temperature, while keeping other simulation assumptions constant. It can be seen from the figures that the exergy destruction and the entropy generation are almost constant in the pump and the expander, while increasing in the gas heater as well as in the gas cooler & condenser with the increasing heat source temperature at the gas cooler inlet. Furthermore, it can be noted from the figure that both the mean temperature difference in the gas heater and the pinch temperature in the gas cooler & condenser increase, while the increment is more obvious in the gas cooler & condenser. As a consequence, although the exergy destruction and the entropy generation increase in both gas heater and the gas cooler & condenser, the increments are more obvious in the gas cooler & condenser than in the gas heater. 70PDF Image | Thermodynamic Cycles using Carbon Dioxide
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