Test case HOM14: Rotating turbulence with plane strain, data from Leuchter et al. (1992)


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

 - longitudinal position x (m),

 - relative position xi=x/L,

 - 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=-2D.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           x/L         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  0.991E+01  0.221E+00  0.155E+00  0.154E+00 -0.555E-02 0.158E+02  0.685E-02  0.319E-02  0.336E-02
  0.3625E-01  0.3125E-01  0.991E+01  0.182E+00  0.128E+00  0.128E+00 -0.110E-01 0.107E+02  0.676E-02  0.379E-02  0.387E-02
  0.7250E-01  0.6250E-01  0.992E+01  0.155E+00  0.110E+00  0.111E+00 -0.131E-01 0.767E+01  0.705E-02  0.431E-02  0.386E-02
  0.1087E+00  0.9375E-01  0.991E+01  0.137E+00  0.947E-01  0.100E+00 -0.150E-01 0.584E+01  0.694E-02  0.491E-02  0.466E-02
  0.1450E+00  0.1250E+00  0.987E+01  0.121E+00  0.833E-01  0.928E-01 -0.153E-01 0.455E+01  0.725E-02  0.534E-02  0.491E-02
  0.1812E+00  0.1562E+00  0.979E+01  0.108E+00  0.736E-01  0.862E-01 -0.162E-01 0.372E+01  0.724E-02  0.599E-02  0.469E-02
  0.2175E+00  0.1875E+00  0.975E+01  0.101E+00  0.665E-01  0.841E-01 -0.173E-01 0.320E+01  0.733E-02  0.649E-02  0.482E-02
  0.2537E+00  0.2187E+00  0.966E+01  0.925E-01  0.594E-01  0.794E-01 -0.163E-01 0.267E+01  0.726E-02  0.662E-02  0.514E-02
  0.2900E+00  0.2500E+00  0.960E+01  0.871E-01  0.545E-01  0.771E-01 -0.164E-01 0.236E+01  0.736E-02  0.735E-02  0.479E-02
  0.3262E+00  0.2812E+00  0.951E+01  0.831E-01  0.509E-01  0.765E-01 -0.165E-01 0.213E+01  0.734E-02  0.758E-02  0.469E-02
  0.3625E+00  0.3125E+00  0.945E+01  0.785E-01  0.469E-01  0.732E-01 -0.175E-01 0.200E+01  0.725E-02  0.746E-02  0.449E-02
  0.4350E+00  0.3750E+00  0.939E+01  0.746E-01  0.458E-01  0.724E-01 -0.174E-01 0.174E+01  0.754E-02  0.829E-02  0.500E-02
  0.5075E+00  0.4375E+00  0.945E+01  0.707E-01  0.459E-01  0.710E-01 -0.200E-01 0.170E+01  0.747E-02  0.808E-02  0.492E-02
  0.5800E+00  0.5000E+00  0.965E+01  0.699E-01  0.491E-01  0.701E-01 -0.213E-01 0.159E+01  0.797E-02  0.855E-02  0.527E-02
  0.6525E+00  0.5625E+00  0.980E+01  0.704E-01  0.534E-01  0.708E-01 -0.230E-01 0.157E+01  0.853E-02  0.884E-02  0.528E-02
  0.7250E+00  0.6250E+00  0.987E+01  0.716E-01  0.550E-01  0.703E-01 -0.225E-01 0.144E+01  0.920E-02  0.859E-02  0.583E-02
  0.7975E+00  0.6875E+00  0.994E+01  0.736E-01  0.586E-01  0.691E-01 -0.222E-01 0.134E+01  0.965E-02  0.830E-02  0.612E-02
  0.8700E+00  0.7500E+00  0.100E+02  0.755E-01  0.602E-01  0.698E-01 -0.209E-01 0.119E+01  0.946E-02  0.822E-02  0.651E-02
  0.9425E+00  0.8125E+00  0.101E+02  0.758E-01  0.577E-01  0.688E-01 -0.187E-01 0.101E+01  0.951E-02  0.854E-02  0.712E-02
  0.1015E+01  0.8750E+00  0.101E+02  0.776E-01  0.565E-01  0.696E-01 -0.176E-01 0.915E+00  0.988E-02  0.869E-02  0.722E-02
  0.1087E+01  0.9375E+00  0.982E+01  0.767E-01  0.497E-01  0.701E-01 -0.164E-01 0.876E+00  0.101E-01  0.101E-01  0.754E-02
  0.1160E+01  0.1000E+01  0.929E+01  0.794E-01  0.426E-01  0.718E-01 -0.179E-01 0.109E+01  0.987E-02  0.104E-01  0.715E-02