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geothermal power plant projects in central america - Orkustofnun

geothermal power plant projects in central america - Orkustofnun

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pressures (kPa) <strong>in</strong> the separator for SF and DF cases and <strong>in</strong> the boiler for the ORC case. In order tosimplify read<strong>in</strong>g from the graphs, the optimum net <strong>power</strong> output (kW) for a unit mass flow rate isused; the total <strong>power</strong> output can be obta<strong>in</strong>ed for each specific case simply by multiply<strong>in</strong>g this by theactual mass flow rate <strong>in</strong> kg/s.4.3.1 S<strong>in</strong>gle flashThe selection of the separatorpressure has an important effect onthe overall <strong>plant</strong> performance <strong>in</strong>terms of <strong>power</strong> output (Figure 19).High separator pressures result <strong>in</strong>higher work<strong>in</strong>g potential steam atthe turb<strong>in</strong>e <strong>in</strong>let, a lower quality ofsteam <strong>in</strong> the turb<strong>in</strong>e exhaust andhigher <strong>in</strong>jection temperature.Lower separator pressures <strong>in</strong>creasethe mixture quality <strong>in</strong> the separator,which means that more steam canbe produced, but the specificavailable energy of the steam flowwould decl<strong>in</strong>e.The optimization rout<strong>in</strong>e isrelatively simple s<strong>in</strong>ce there is onlyone optimization variable and it canbe determ<strong>in</strong>ed by vary<strong>in</strong>g the valueof the wellhead pressure to locatethe <strong>power</strong> output maximum(Karlsdóttir, 2008). The results ofthe optimization process arepresented <strong>in</strong> Figure 20 as theoptimum specific net output and theseparator pressure (kPa) as afunction of the resourcestemperature. The specific net <strong>power</strong>output is directly proportional tothe resource temperature. Theseparator pressure <strong>in</strong>creases for aresource temperature rang<strong>in</strong>g from160 to 280°C; for higher resourcevalues it is constant as the constra<strong>in</strong>ts of the steam quality of the turb<strong>in</strong>e exhaust cannot be lower than0.85, as seen <strong>in</strong> Figure 20.4.3.2 Double flashSpecific <strong>power</strong> output [ kW/kg/s ]Specific net <strong>power</strong> output [ kW/kg/s ]3002502001501005030025020015010000160 180 200 220 240 260 280 300 320 340Resource temperature [°C]50Specific net <strong>power</strong> outputSeparator pressureFIGURE 4: Specific net <strong>power</strong> output and separatorpressure of SF cycleSpecific net <strong>power</strong> outputSteam quality at turb<strong>in</strong>e output00.70160 180 200 220 240 260 280 300 320 340Resource temperature [ °C ]In the optimization process of a DF cycle, the maximum <strong>power</strong> output is gotten by adjust<strong>in</strong>g the valueof the high-pressure (HP) and low-pressure (LP) separators. Also, <strong>in</strong> a DF cycle, as <strong>in</strong> a SF cycle, thesteam quality of the turb<strong>in</strong>e exhaust is a constra<strong>in</strong>t <strong>in</strong> the optimization process, <strong>in</strong> this case for twostations at the exhaust of LP and HP turb<strong>in</strong>es (Figure 22).Figure 21 shows the optimum specific net output and pressure separation for different resourcetemperatures. The specific net <strong>power</strong> output and the optimum pressure value of the HP separator aredirectly proportional to the temperature resource. In the DF system, as shown <strong>in</strong> Table 3, themaximum well head pressure was set at 3500 kPa, correspond<strong>in</strong>g to the HP separator pressure at340°C. Where limits for the maximum well head pressure are set lower, the pressure <strong>in</strong>creases until it8007006005004003002001001.000.950.900.850.800.75FIGURE 4: Specific net <strong>power</strong> output and steam qualityof turb<strong>in</strong>e output of SF cycleSeparator pressure [ kPa ]Steam quality [ - ]24

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