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Table 3 Numerical values of \( -\sqrt{\operatorname{Re}}{C}_f \) and \( -\left[\frac{\mathrm{N}{\mathrm{u}}_x}{\mathrm{R}{\mathrm{e}}^{1/2}}\right] \) for different values of We, n, M, β v , and l

From: Flow and heat transfer of dusty hyperbolic tangent fluid over a stretching sheet in the presence of thermal radiation and magnetic field

M We β v l n \( -\sqrt{\operatorname{Re}}{C}_f \) \( -\left[\frac{\mathrm{N}{\mathrm{u}}_x}{\mathrm{R}{\mathrm{e}}^{1/2}}\right] \)
0      1.0547 1.0506
0.5      1.2641 1.0115
1      1.4446 0.9788
  0     1.2247 1.0137
  0.3     1.2641 1.0115
  0.6     1.3057 1.0093
   0.5    1.2641 1.0115
   1    1.2958 0.9956
   1.5    1.3144 0.9834
    0.5   1.2641 1.0115
    1   1.3268 1.1973
    1.5   1.3868 1.3598
     0 1.2440 1.1973
     0.1 1.2909 1.0257
     0.2 1.3268 0.9942