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(Figure 2‐1). In this system, the carbon dioxide is first pumped to a supercritical pressure, and then heated in the gas heater. The heated supercritical carbon dioxide will expand in an expansion machine (e.g. a turbine). The vapor discharged from the expansion machine outlet will then be cooled and condensed in a condenser (gas cooler). An Internal Heat Exchanger (IHX, regenerator) can be added to the basic system to optimize the system performance. The importance of utilizing a regenerator in a carbon dioxide transcritical power cycle will be shown in the latter part of this thesis. Figure 2‐1 Schematic of the carbon dioxide power system (for both Brayton cycle and transcritical cycle) The corresponding cycles of this system are carbon dioxide transcritical power cycle and carbon dioxide Brayton cycle respectively. Both cycles consist of four processes, namely: compression (a‐b), isobaric heat supply (b‐d), expansion (d‐e), isobaric heat rejection (e‐a). The only difference between these two cycles is whether part of the cycle is located in the sub‐ critical region or not. Therefore, both cycles are sometimes 13PDF Image | Thermodynamic Cycles using Carbon Dioxide
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