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Generating Power Using Geothermal Resources                                 165


            sTeam qualiTy
            One of the important factors influencing the performance of a generating system is the quality of
            the steam that enters the turbine. Steam quality is defined as the proportion of water vapor to liq-
            uid water in the steam phase. In Figure 9.7, the ratio of vapor-to-liquid in the two-phase region is
            contoured by the dashed lines. As previously noted, Baumann (1921) found that every percentage
            increase in moisture content of the vapor resulted in an approximately 0.5% drop in efficiency. This
            raises an important consideration.
              Remembering that our process is an idealized isenthalpic system, it is clear that we will maxi-
            mize the amount of steam in our system if we reduce the temperature and pressure as much as possi-
            ble. We will assume the final state will be 50°C (point 2 in Figure 9.7). For isentropic conditions, the
            steam enthalpy would be 1980 kJ/kg and the realized enthalpy will be 2166 kJ/kg as before. From
            mass balance relationships discussed earlier in Chapter 3, we find that about 33% of the fluid mass
            is converted to steam (point 3 in Figure 9.7). Hence, for every kilogram of steam we must extract
            three kilograms of liquid from the reservoir. Since each kilogram of liquid has an enthalpy of 1085
            kJ/kg, we must extract 3245 kJ from the reservoir to obtain 638 kJ of work from the available steam.
            As noted previously, moisture reduces turbine efficiency, and yet in this situation, two-thirds of the
            mass of the system remains as liquid water. If this were to enter the turbine, the efficiency of our
            energy extraction process would be diminished by about 30%, which would be an unacceptable loss
            in generating capacity.
              It is crucial to have the ability to separate liquid from vapor in any hydrothermal resource. For
            this purpose a cyclone separator (Figure 9.10) is placed between the turbine and the wellhead. The
            high-pressure mixed vapor–liquid phase that exits the wellhead is piped to the separator where,
            through a combination of gravity and centrifugal effects, liquid separates from the vapor. The veloc-
            ity at the inlet pipe is commonly maintained between 25 m/s and 40 m/s (Lazalde-Crabtree 1984),




                                                    Dry steam







                                    Inlet for
                                    wet steam                       Water
                                  from wellhead                    droplets










                              Liquid water
                              to collector
                                                               Dry steam
                                                               to turbine

            FIGUre 9.10  Schematic representation of a cyclone separator. Mixed vapor and liquid enter at high velocity
            and flow through the open volume. Centrifugal effects cause the liquid to impact the interior surface and flow
            down the sides of the separator, collecting and draining at the bottom. The resulting dry steam exits through
            the high stand pipe and is piped to the turbine.
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