Page 82 - Low Temperature Energy Systems with Applications of Renewable Energy
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Characteristics of low-temperature energy sources for heat pumps   71

           Thus, it is desirable to use other characteristics to find the efficiency of the entire sys-
           tem. Therefore, in the following analysis the value of specific losses of external energy
           are determined for the heat supply system, which, in case of energy losses for only the
           heat pump, is a value different from the heat pump COP.
              In general the total specific losses of external energy l h for the heat pump and
           ambient coolant driver of a low-temperature heat carrier can be presented in the
           following way:


                   L tot  L c þ L m$e
                              s
                l h ¼  ¼         ;                                         (2.9)
                    Q h     Q c
           where L c , L m$e  are energy losses for a heat pump compressor and ambient coolant
                     s
           driver, respectively, kW; Q c is the heat flow extracted from the heat pump condenser,
           kW.
              Energy losses for the heat pump L c are defined by the equation:


                     Q ev
               L c ¼    :                                                 (2.10)
                    4   1
              Heat flow in the heat pump evaporator Q ev is given by:

                             in  out
               Q ev ¼ V s r c p t s    t s  ;                             (2.11)
                        s
           where V s , r s , and c p are volume loss, density and isobaric specific heat of the sur-
                               in
           roundings, respectively; t , t out  , are surroundings temperatures at the evaporator inlet
                               s  s
           and outlet, respectively.
              Energy losses for ambient coolant driver are:

                      V c Dp
                m:e
               L   ¼       ;                                              (2.12)
                s     m:e
                     h  h
                      s   dr
           where Dp is aerodynamic and hydraulic pressure losses at the heat pump evaporator
           that depend on the chosen energy source; in the case of using soil heat,
           Dp ¼ Dp ev þ Dp s.h , namely, total pressure drop in the lower loop (in the heat pump
           evaporator and soil heat exchanger); h m:e  and h are the efficiency of ambient coolant
                                         s      dr
           driver and its motor, respectively. One can assume that at the optimum operating point
           h m:e  ¼ 0:8 for a fan and pump, and the driver motor efficiency, h dr ¼ 0.95.
            s
              Heat flow Q c in Eq. (2.9) is determined from the HP heat balance equation:

               Q c ¼ Q ev þ L c                                           (2.13)
              The actual COP of the heat pump 4 can be presented in the following way:

               4 ¼ 4 h  ;                                                 (2.14)
                    t HP
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