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250                 Low-Temperature Energy Systems with Applications of Renewable Energy

         Table 6.4 Temperatures and mass flow rates at key points in the system shown in Fig. 6.22.

                                        Temperature,   Mass flow,  Mass flow,
          Location  Item                8C             t/h        kg/s
          1        Exchange water       15             710        197.2
          2        Geothermal brine     145            1000       277.8
          3        Produced hot water   115            800        222.2
          4        Fresh water for dilution  w15       250        69.4
          5        Industrial consumption  115         300        83.3
          6        Residential & general  85           750        208.3
                     usage





















         Fig. 6.24 Kakkonda-Shizukuishi HWPF in 1986, looking generally south; photo by R. DiPippo.
         Five upper steam pipes run from the flash evaporator (horizontal vessel at top rear) to the direct-
         contact heat exchanger (horizontal vessel middle). The vertical vessel at the right is a deaerator.


         steam at ever lower temperatures which heats fresh water from the Kakkonda River via
         five heat exchangers, four of which are direct contact type (see Fig. 6.25). Thus, the
         treated river water mixes with the flash steam to form hot water of sufficient purity
         for municipal use.
            The process flow diagram for the overall system is shown in Fig. 6.25. Multiple pro-
         duction, injection, and fresh water wells were used.
            The utilization efficiency of the HWPF can be calculated based on the exergy of the
         separated brine coming from the power plant and the exergy of the hot water sent to the
         heating districts. From Table 6.4, the ratio of the exergy rate at location 3 to that at

         location 2 is a measure of the efficiency. Thus, using a 15 C dead state, we find
                  _
                  E 3  13; 234:1
             h ¼     ¼         ¼ 0:495                                  (6.40)
              U   _
                  E 2  26; 730:8
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