Page 48 - Introduction to Computational Fluid Dynamics
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                        2.5 STABILITY AND CONVERGENCE
                        Table 2.1: Explicit procedure with ∆t = 10 s (stable).     May 25, 2005  10:49  27
                        Time     0 mm    1 mm     3 mm     5 mm      7 mm     9 mm     10 mm
                          0      250      30       30       30        30       30      250
                         10      250     135.7     30       30        30      135.7    250
                         20      250     165.3     55.43    30        55.43   165.3    250
                         30      250     179.6     75.72    42.22     75.22   179.6    250
                         40      250     188.5     92.5     58.33     92.5    188.5    250
                         50      250     195.0    107.4     74.82    107.4    195.0    250
                         60      250     200.4    120.6     90.5     120.6    200.4    250
                         70      250     205.1    132.6    105.0     132.6    205.1    250
                         80      250     209.3    143.4    118.3     143.4    209.3    250
                         90      250     213.0    153.2    130.3     153.2    213.0    250
                        100      250     216.4    162.1    141.3     162.1    216.4    250


                        q = 0. We solve this problem by an explicit method (ψ = 0) and employ the IOCV

                        method. 5
                           We now note that ρ A i  x i C = 1,300 × 1 × 0.002 × 2,000 = 5,200, AW 2 =
                        0.25 × 1/0.001 = 250, AW i = 0.25 × 1/0.002 = 125 for i = 3to N − 1,
                         AE N−1 = 0.25 × 1/0.001 = 250, and AE i = 0.25 × 1/0.002 = 125 for i = 2to
                         N − 2. Therefore, the applicable discretised equations are

                                     5,200           o        o    5,200          o
                                           T 2 = 250 T + 125 T +         − 375 T ,         (2.33)
                                                     1
                                                                                 2
                                                             3
                                        t                            t
                                     5,200         
  o     o       5,200         o
                                           T i = 125 T  + T     +        − 250 T ,         (2.34)
                                       t             i−1    i+1       t           i
                        for i = 3, 4, and 5 and
                                  5,200             o          o     5,200         o
                                       T N−1 = 125 T N−2  + 250 T +       − 375   T N−1 .  (2.35)
                                                               N
                                    t                                 t
                           Finally, the boundary conditions are T 1 = 250 and T N = 250. These conditions
                        apply because it is assumed that when the sheets are pressed, the thermal contact
                        between the sheets and the pressing surface is perfect.
                           This set of discretised equations dictates that  t must be less than 5,200/375 =
                        13.87 s (see Equation 2.32). We therefore carry out two sets of computations, one in
                        which  t = 10 s (see Table 2.1) and another in which  t = 20 s, so that the stability
                        condition is violated (see Table 2.2). In both cases, computations are stopped when
                                                 ◦
                        T 4 (x = 5 mm) exceeds 140 C.
                           Table 2.1 clearly shows monotonic evolution of temperature within the sheets
                        and thus accords with our expectation. The time for which the two sheets should

                        5  Note that because in this problem kA is constant, the coefficients AE i , AW i , and AP i will be
                          identical in both the IOCV and TSE methods.
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