Page 92 - Sustainable On-Site CHP Systems Design, Construction, and Operations
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70    CHP B a s i c s


                   20.000
                                       LT HW        HT HW       15-psig steam
                   18.000
                   16.000
                  Heat recovered (MBH)  12.000
                   14.000


                   10.000
                    8.000
                    6.000
                    4.000
                    2.000
                    0.000
                          75  255  375  450  600  750  769  770  980  1100  1100  1200  1250  1400  1750  2055  2615  3480  5238

                                              Engine output (kW)
             FIGURE 4-3  Heat recovery versus heat quality for various reciprocating engines. (Courtesy of
             Integrated CHP Systems Corporation.)



                For reciprocating engine–based systems, the thermal product quality required by
             the building can have a dramatic effect on heat recovery. Figure 4-3 gives the heat recovery
             potential for a variety of reciprocating engines based on the quality of thermal product
             required. For example, if a facility requires 15 psig or higher-pressure steam or over
             240°F hot water, then most engines will not be able to incorporate the jacket loop into
             the heat recovery process resulting in the inability to recover approximately 50 percent
             of the waste heat available.
                For engines whose thermal output is in the form of exhaust only such as com-
             bustion turbines and some fuel cells, the main parameter for calculating the heat
             recovery potential is product quality requirements. Reciprocating engines present a
             particular difficulty as illustrated above in providing two distinctly different forms
             of thermal energy—hot water/glycol through the various engine cooling loops and
             high temperature exhaust from the engine stack. While each thermal output can be
             recovered separately, it is often more economically efficient to recover both outputs
             into a single stream. This is done by passing the engine coolant after it leaves the
             block through an air-to-liquid heat exchanger and recovering the exhaust energy
             into the coolant loop, resulting in an increase in temperature. This is especially true
             for smaller reciprocating engines where the jacket coolant loop represents a higher
             portion of the thermal output than the exhaust stream and the cost of exhaust heat
             recovery is unreasonable for such small volumes. As depicted in Fig. 4-4, the com-
             bined electric and thermal efficiency for reciprocating engines is fairly constant for
             all but the smallest engines. This figure also demonstrates the potential to obtain up
             to 80 percent fuel efficiency from CHP systems when all potential heat output is
             recovered. As the engines get bigger, electric efficiency increases while the thermal
             efficiency decreases. The efficiencies depicted in Fig. 4-4 are based on the higher
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