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DEVELOPMENT OF A SUPERCRITICAL CO2 BRAYTON ENERGY

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DEVELOPMENT OF A SUPERCRITICAL CO2 BRAYTON ENERGY ( development-supercritical-co2-brayton-energy )

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CHAetal., DevelopmentofaSupercriticalCO2BraytonEnergyConversionSystemCoupledwithaSodiumCooledFastReactor Fig. 15. MMS-LMR Model of KALIMER-600 with a Brayton Cycle Table 12. Summary of the Steady State Calculation Parameters Reference Result Unit Reactor power 100% 100.08 % Temperature at core inlet/outlet 390/545 390.2/545.3 oC PHTS flow rate 7731.3 7732.5 kg/sec Temperature at IHX inlet/outlet in IHTS 364.0/526.0 364.1/526.1 oC IHTS flow rate 7400.2 7401.9 kg/sec Temperature at Na-CO2 HEX S-CO2 cycle 353.8/508 353.9/508 oC Temperature at turbine outlet 394.2 394.8 oC Temperature at HTR Hot side Cold side 394.2/203.1 185.8/353.9 394.8/204.9 192.6/353.8 oC oC Temperature at LTR Hot side Cold side 203.1/91.20 84.8/184.2 204.9/85.6 68.2/167.8 oC oC Pressure at HTR Hot side Cold side 7.6/7.53 19.98/19.94 7.59/7.46 19.83/19.79 MPa MPa Pressure at LTR Hot side Cold side 7.53/7.46 20.0/19.98 7.46/7.4 19.85/19.83 MPa MPa Flow rate in S-CO2 cycle Compressor 1 side Compressor 2 side 8076.6 5734.42 2342.21 8076.7 5707.0 2369.8 kg/sec kg/sec kg/sec power operation of the KALIMER-600. There are some differences in temperatures for the cold side LTR; these could be overcome by further study of S-CO2 compressors’ data. Then, the transient behavior was analyzed for the KALIMER-600 with S-CO2 Brayton cycle. A simple power reduction and recovery event was chosen for the transient analysis. The analysis results were more or less NUCLEAR ENGINEERING AND TECHNOLOGY, VOL.41 NO.8 OCTOBER 2009 1039

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