Test case HOM20: Transversely sheared flow, data from Leuchter et al. (1990, 1991)


The results are displayed in a table with 11 columns corresponding to the
following quantities:

 - longitudinal position x (m),

 - non-dimensional time St

 - axial mean velocity component U (m/s),

 - Reynolds stresses u^2, v^2, w^2, vw (m^2/s^2)

 - dissipation rate epsilon (m^2/s^3), evaluated from epsilon=-S.vw-1/2.U.dq^2/dx,

 - lengthscales L_u (= L_11,1), L_v (= L_22,1), L_w (= L_33,1) (m).


     x           Dt          U          u^2        v^2        w^2        vw      epsilon     L_u        L_v        L_w
    (m)                    (m/s)     (m^2/s^2)  (m^2/s^2)  (m^2/s^2)  (m^2/s^2) (m^2/s^3)    (m)        (m)        (m)

  0.0000E+00  0.0000E+00  0.996E+01  0.229E+00  0.147E+00  0.144E+00 -0.179E-02 0.160E+02  0.659E-02  0.263E-02  0.278E-02
  0.5499E-01  0.1875E+00  0.994E+01  0.169E+00  0.126E+00  0.104E+00  0.332E-02 0.962E+01  0.719E-02  0.260E-02  0.304E-02
  0.1100E+00  0.3751E+00  0.996E+01  0.133E+00  0.832E-01  0.831E-01 -0.754E-02 0.591E+01  0.747E-02  0.308E-02  0.318E-02
  0.1650E+00  0.5626E+00  0.100E+02  0.113E+00  0.710E-01  0.716E-01 -0.109E-01 0.407E+01  0.785E-02  0.323E-02  0.333E-02
  0.2200E+00  0.7502E+00  0.100E+02  0.974E-01  0.608E-01  0.640E-01 -0.129E-01 0.292E+01  0.798E-02  0.351E-02  0.345E-02
  0.2750E+00  0.9377E+00  0.102E+02  0.893E-01  0.620E-01  0.600E-01 -0.149E-01 0.232E+01  0.774E-02  0.361E-02  0.349E-02
  0.3300E+00  0.1125E+01  0.102E+02  0.792E-01  0.528E-01  0.558E-01 -0.138E-01 0.174E+01  0.785E-02  0.411E-02  0.374E-02
  0.3850E+00  0.1313E+01  0.103E+02  0.736E-01  0.482E-01  0.550E-01 -0.159E-01 0.148E+01  0.799E-02  0.467E-02  0.416E-02
  0.4400E+00  0.1500E+01  0.103E+02  0.684E-01  0.451E-01  0.535E-01 -0.164E-01 0.128E+01  0.797E-02  0.474E-02  0.413E-02
  0.4950E+00  0.1688E+01  0.103E+02  0.648E-01  0.545E-01  0.507E-01 -0.177E-01 0.120E+01  0.792E-02  0.434E-02  0.414E-02
  0.5500E+00  0.1875E+01  0.103E+02  0.618E-01  0.410E-01  0.526E-01 -0.173E-01 0.106E+01  0.803E-02  0.532E-02  0.417E-02
  0.6050E+00  0.2063E+01  0.104E+02  0.590E-01  0.394E-01  0.530E-01 -0.181E-01 0.101E+01  0.793E-02  0.577E-02  0.431E-02
  0.6600E+00  0.2251E+01  0.105E+02  0.579E-01  0.392E-01  0.540E-01 -0.193E-01 0.999E+00  0.787E-02  0.604E-02  0.434E-02