Page 283 - Process Modelling and Simulation With Finite Element Methods
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270         Process Modelling and Simulation with Finite Element Methods

                                    MBX  0752                         Max 0 0513
             Time=O 001  Contour  concentration of c   Time.0   06  Contour  concentration ofc
                                      07163   I'                     I   0 0501
                                      0 6805                           0 0489
                                      0 6447                           0  0 0477 0466
                                      0 6089
                                      0 5731
                                      0 5373                           0 0453
                                                                       0 M4l
                                                                       0
                                                                        043
                                      0 5014
                                      0 4656
                                      0 4298                           0 0418
                                                                       0 0406
                                      0 394                            0 0394
                                      0 3552                           0 0382
                                      3224
                                      0
                                                                       0
                                                                        037
                                      0 28s5                           0 0358
                                      0 2507                           0 0346
                                      02149                            0 0334
                                                                        031
                                      0 1791                           0  0 0322
                                      01433
                                      0 1075
                                      00716
                                                                       0 0238
                                                                        0274
                                      0 0358                           0  0 0286
                                            I,                       I
                                    Mm  2,380,   05   0   05   1    15   hln  0 "252
         Figure 7.8  Isopycnals  for times  t=0.001  (left)  and  t=0.06  (right)  for  the time  evolution  of  the
         concentration  field  from  cg  (7.1 1)  according  to  the  convective-diffusion  model  with  Pe=l  and
         uniform horizontal flow under doubly periodic boundary conditions.
         The latter  two  give  s,=0.0707 and  s,=0.0872,  consistent  with  the  settings of 1,
         and 1,  as expected.
                 Time=0.06,  projl on bnd 2         Time=0.06,  proj2 on bnd 1
                                             0 042 1
           0 045                             0 044 r
          Q
           0 035
                                             0 034
                                             0 032
                                                                  '
                                                       '
                          '
           0031   " "        '  1  '   "     003l   "       "       '     ,
             0   01   02   03   04   05   06   07  08   09   1   0   01   02   03   04   05   06   07   08   09   1
                      x-coordinate                      y-coordinate
         Figure 7.9  Line  integral  projections  for t=0.06  onto  the  horizontal  boundary  (left)  and  vertical
         boundary (nght) for the model of Figure 7.8.
         Figure 7.8 shows the extent to which the initial condition  diffuses very rapidly.
         Although the Pe=l  in this  simulation, the numerical diffusivity  is strong on this
         mesh resolution.  Likely the result is less rapid diffusion on a finer mesh.  Figure
         7.9  gives  the  projection  coupling  variables  demonstrating  the  near  Gaussian
         profiles captured by our synthetic "lidar."  Clearly, even the late stage evolution
         where  periodic  boundary  conditions  obscure  the  usual  "long  tails"  of  the
          Gaussians,  exhibit  a  central  peak  and  spread  captured  by  the  central  moments
          according to (7.14) and (7.15).
         Exercise  7.3: Artificial (numerical) diffusivity
         Repeat the lidar example with a refined mesh.  Does the Gaussian cloud disperse
         slower (less spread) with a refined mesh.  How could you use this computation to
         quantify the numerical diffusivity that is artificially created?
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