Table 1 Numerical values of Drag force \(C_{f} {\text{Re}}_{x}^{1/2}\) against the varied values of the rising parameter.

From: Significance of Hall effect and Ion slip in a three-dimensional bioconvective Tangent hyperbolic nanofluid flow subject to Arrhenius activation energy

\(M\)

\(Ec\)

\(\Pr\)

\(We\)

\(\beta_{e}\)

\(\beta_{i}\)

\(- \sqrt {\text{Re}} C_{fx}\)

\(- \sqrt {\text{Re}} C_{gy}\)

0

3

3

1

1.2

0.9

1.3748921

0.70471084

0.5

     

1.3891760

0.72841397

0.7

     

1.4028943

0.75088802

0.9

     

1.4211882

0.78043358

0.5

1

    

1.3891760

0.72841397

 

2

    

1.3891760

0.72841397

 

3

    

1.3891760

0.72841397

 

4

    

1.3891760

0.72841397

 

3

1

   

1.3891764

0.72841397

  

2

   

1.3891764

0.72841397

  

3

   

1.3891764

0.72841397

  

4

   

1.3891764

0.72841397

  

3

1

  

1.389176

0.72841397

   

2

  

1.3117802

0.70827679

   

3

  

1.2240033

0.68654032

   

4

  

0.78790504

0.67413247

   

1

0.6

 

1.4005879

0.73505713

    

1

 

1.3918829

0.73046773

    

1.5

 

1.3862657

0.72576016

    

2.1

 

1.3827605

0.72175107

    

1.2

0.2

1.3861825

0.74221885

     

0.5

1.3885132

0.73530222

     

0.7

1.3890701

0.73155041

     

0.9

1.3891760

0.72841397

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