A Novel Numerical Technique for Two-Dimensional Laminar Flow between Two Moving Porous Walls

Table 2

Comparison of the numerical results against the SHAM approximate solutions for $F^{\prime \prime }(1)$ when $\alpha =-1$ with $N=60$ and $\hslash =-1$ for different values of $\mathrm{Re}$.

$\mathrm{Re}$	0th order	1st order	2nd order	3rd order	4th order	Numerical
0	−3.8213722	−3.8213723	−3.8213723	−3.8213723	−3.8213723	−3.8213723
5	−3.1725373	−3.1731774	−3.1731800	−3.1731800	−3.1731800	−3.1731800
10	−2.9069253	−2.9069653	−2.9069654	−2.9069654	−2.9069654	−2.9069654
15	−2.7783086	−2.7784366	−2.7784369	−2.7784369	−2.7784369	−2.7784369
20	−2.7056150	−2.7060556	−2.7060557	−2.7060557	−2.7060557	−2.7060557
25	−2.6596223	−2.6603920	−2.6603907	−2.6603907	−2.6603907	−2.6603907
30	−2.6281102	−2.6291718	−2.6291682	−2.6291682	−2.6291682	−2.6291682
40	−2.5879160	−2.5894333	−2.5894247	−2.5894247	−2.5894247	−2.5894247
50	−2.5634446	−2.5652868	−2.5652732	−2.5652733	−2.5652733	−2.5652733
100	−2.5139141	−2.5165255	−2.5164964	−2.5164967	−2.5164967	−2.5164967
150	−2.4972813	−2.5001845	−2.5001479	−2.5001484	−2.5001484	−2.5001484