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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