Page 299 - Fundamentals of The Finite Element Method for Heat and Fluid Flow
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SOME EXAMPLES OF FLUID FLOW AND HEAT TRANSFER PROBLEMS


                                   (a) q = 0°, Re = 100  (b) q = 0°, Re = 200  (c) q = 0°, Re = 300  291







                                   (d) q = 10°, Re = 100  (e) q = 10°, Re = 200  (f) q = 10°, Re = 300








                                   (g) q = 20°, Re = 100  (h) q = 20°, Re = 200  (f) q = 20°, Re = 300

                        Figure 9.33 Forced convection heat transfer from spherical heat sources mounted on the
                        wall. Temperature contours from the staggered arrangement for different inclination angles
                        and Reynolds numbers

                           Figure 9.33 shows the temperature contours for the staggered arrangement (top view)
                        at different values of Re and angles θ of the inlet flow. It is seen that close packaging
                        reduces the fluid penetration and thus the convection of the temperature in the vicinity
                        of the cluster. In fact, the temperature gradients in the zone occupied by the balls are
                        almost nil, and this is shown by the uniformity of the isothermal area at the centre of
                        the packaging. The flow encounters several columns of balls in a staggered arrangement
                        and therefore decelerates drastically after the first column. By increasing the velocity of
                        the fluid (Reynolds number), it is obviously possible to increase the temperature gradients
                        between the balls and the cooling fluid. As shown in Figure 9.33, for an angle of 0 ,the
                                                                                             ◦
                        cooling fluid penetrates further into the packaging as the velocity increases. However, this
                        is achieved at the cost of a large increase in the energy necessary to speed up the fluid. As
                        for the case of the in-line arrangement, the fluid penetration increases with both Reynolds
                        number and angle of attack. For the same intensity of fluid penetration into the cluster, the
                        staggered arrangement needs a much higher Reynolds number and angle of attack than that
                        of the in-line arrangement.
                           Before discussing the surface Nusselt number variation over the heat sources, it is
                        useful to define some keywords in order to identify the heat sources. Figure 9.34 gives
                        some definitions in order to explain the Nusselt numbers. These keywords will be referred
                        to in the following paragraphs.
                           In Figure 9.35, the average Nusselt number is presented for the central and the lateral
                        rows of balls for in-line arrangement (refer to Figure 9.34 for ‘lateral’ and ‘central’ rows).
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