Energy Conversion Systems

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Energy Conversion Systems ( energy-conversion-systems )

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7.2.3 Electricity from EGS resources at supercritical conditions Energy Conversion Systems – Options and Issues SPT F LPCT The analysis was based on the following assumptions: Chapter 7 A novel energy conversion system was developed to handle the cases when the EGS geofluid arrives at the plant at supercritical conditions, i.e., at a temperature greater than 374°C and a pressure greater than 22 MPa. For all situations studied, the temperature was taken as constant at 400°C. The plant is called the “triple­expansion” system; it is shown in simplified schematic form in Figure 7.11, and the thermodynamic processes are shown in the temperature­entropy diagram in Figure 7.12. The triple­expansion system is a variation on the conventional double­flash system, with the addition of a “topping” dense­fluid, back­pressure turbine, shown as item SPT in Figure 7.11. The turbine is designed to handle the very high pressures postulated for the EGS geofluid, in much the same manner as a “superpressure” turbine in a fossil­fueled supercritical double­reheat power plant (El Wakil, 1984). However, in this case, we impose a limit on the steam quality leaving the SPT to avoid excessive moisture and blade erosion. 7­17 S WV 1 CS HPT 89 BCV5 7 TV 6 3 11 CW • Geofluid inlet temperature, T = 400°C. • Geofluid pressure, P1 > 22 MPa. • Condenser temperature and pressure: T10 = 50°C and P10 = 0.123 bar = 0.0123 MPa. • All turbine and pump isentropic efficiencies are 80%. • Steam quality at SPT exit, state 2 = 0.90. • HPT­ and LPT­turbine outlet steam qualities (states 8 and 10) are unconstrained. 4 13 PW21 HPP 12 14 IW To determine the “optimum” performance, we selected the temperature at the outlet of the flash vessel (state­point 5) as the average between the temperature at the SPT outlet (state 2) and the condenser (state 10), in accordance with the approximate rule­of­thumb for optimizing geothermal double­flash plants (DiPippo, 2005). No claim is made, however, that this will yield the true optimum triple­ expansion design, but it should not be far off. Figure 7.11 Triple­expansion power plant for supercritical EGS fluids. LPP 10

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