Page 35 - Fundamentals of The Finite Element Method for Heat and Fluid Flow
P. 35

SOME BASIC DISCRETE SYSTEMS
                           Equation 2.31 reduces to Equation 2.14 in the absence of convection from the surface.
                        Also, if the terms (T i + T j )/2 in Equation 2.31 are replaced by (2T i + T j )/3, then we
                        obtain the standard Galerkin weighted residual form discussed in Example 3.5.1.  27
                        2.2.4 Analysis of a heat exchanger
                        The performance of a heat exchanger can be calculated in terms of its effectiveness for
                        a given condition (Holman 1989; Incropera and Dewitt 1990). In order to determine the
                        effectiveness of a heat exchanger, we have to calculate the outlet temperatures of both
                        the hot fluid and the cold fluid for the given inlet temperatures. The overall heat transfer
                        coefficient may be a constant or could vary along the heat exchanger.
                           For the purpose of illustration, let us consider a shell and tube heat exchanger as shown
                        in Figure 2.6 (Ravikumaur et al. 1984). In this type of heat exchanger, the hot fluid flows
                        through the tube and the tube is passed through the shell. The cooling fluid is pumped into
                        the shell and thus the hot fluid in the tube is cooled.
                           Let us divide the given heat exchanger into eight cells as shown in Figure 2.7. It is
                        assumed that both the hot and cold fluids will travel through the cell at least once. Let the
                        overall heat transfer coefficient be U and the surface area of the tubes be ‘A’. These are
                        assumed to be constant throughout the heat exchanger within each element. Let us assume
                        that the hot and cold fluid temperatures vary linearly along the flow.
                           Now, the heat leaving node 1 and entering element 1 (Figure 2.7b) is

                                                        Q 1 = W 1 T 1                       (2.33)
                        where W 1 is ρc p times the volume flow rate. The heat leaving element 1 and entering node
                        2 is (the energy balance is considered with respect to the element where the heat entering
                        is taken as being positive and that leaving the element is taken as being negative)

                                               Q 2 = W 1 T 1 − UA(T 1,2 − T 11,12 )         (2.34)
                        where
                                                 T 1 + T 2            T 11 + T 12
                                           T 1,2 =       and T 11,12 =                      (2.35)
                                                    2                    2

                                              Cold fluid inlet     Cold fluid exit



                                   Cold fluid out                                Tube


                                   Hot fluid in
                                                                                   Shell


                                                                    Baffles
                                 Figure 2.6 Schematic diagram of a shell and tube heat exchanger
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