Table 8.

Sensitivity analysis with A = 0 and all combination of magnetic parameter and suction parameter for skin friction coefficients $C_{\mathit{fr}}R{e}_r^{1/2}$ , $C_{g{\theta }^{\ast }}R{e}_r^{1/2}$ and the local Nusselt number $N{u}_{r}R{e}_r^{-1/2}$ is presented.

B	C	Sensitivity
		$\frac{\partial {\text{(C}}_{\text{fr}}{\text{Re}}_r^{1/2})}{\partial A}$	$\frac{\partial {\text{(C}}_{\text{fr}}{\text{Re}}_r^{1/2})}{\partial B}$	$\frac{\partial {\text{(C}}_{\text{fr}}{\text{Re}}_r^{1/2})}{\partial B}$	$\frac{\partial {\text{(C}}_{\text{g}\theta }{\text{Re}}_r^{1/2})}{\partial A}$	$\frac{\partial {\text{(C}}_{\text{g}\theta }{\text{Re}}_r^{1/2})}{\partial B}$	$\frac{\partial {\text{(C}}_{\text{g}\theta }{\text{Re}}_r^{1/2})}{\partial C}$	$\frac{\partial {\text{(N}}_{{\text{u}}_{\text{r}}}{\text{Re}}_r^{1/2})}{\partial A}$	$\frac{\partial {\text{(N}}_{{\text{u}}_{\text{r}}}{\text{Re}}_r^{1/2})}{\partial B}$	$\frac{\partial {\text{(N}}_{{\text{u}}_{\text{r}}}{\text{Re}}_r^{1/2})}{\partial C}$
− 1	− 1	0.221444	0.130533	0.089967	− 0.05249	− 0.08565	− 2.93867	0.314588	− 0.00565	0.027213
	0	0.114505	0.082804	0.992033	− 0.27229	− 0.2515	− 3.20555	0.323688	− 0.01078	0.060863
	1	0.007566	0.035075	1.894099	− 0.49209	− 0.41735	− 3.47243	0.332788	− 0.0159	0.094513
0	− 1	0.217801	− 0.04258	0.042238	− 0.06248	− 0.07545	− 3.10452	0.313063	− 0.00415	0.022088
	0	0.110862	− 0.09031	0.944304	− 0.28228	− 0.2413	− 3.3714	0.322163	− 0.00928	0.055738
	1	0.003923	− 0.13804	1.84637	− 0.50208	− 0.40715	− 3.63828	0.331263	− 0.0144	0.089388
1	− 1	0.214158	− 0.2157	− 0.00549	− 0.07247	− 0.06525	− 3.27036	0.311538	− 0.00265	0.016963
	0	0.107219	− 0.26343	0.896575	− 0.29227	− 0.23109	− 3.53725	0.320638	− 0.00778	0.050613
	1	0.00028	− 0.31116	1.798641	− 0.51207	− 0.39694	− 3.80413	0.329738	− 0.0129	0.084263