Table 4 Convergence of HAM solution for different orders of approximation for \(f''(0)\), \(-g'(0)\), \(-h'(0)\), \(-n'(0)\), \(-\theta ' (0)\) and \(-\Psi ' (0)\) when \(\xi _{rad} = 0.1\), \(\xi _{sq} = 0.1\), \(\xi _{z} = 0.2\), \(\xi _{\theta } = 0.5\), \(\xi _{mag} = 0.3\), \(\xi _{pr} = 0.2\), \(\xi _{hm} = 1\), \(\xi _{pm} = 0.2\), \(\xi _{sm} = 1\), \(\xi _{ec} = 0.1\), \(\xi _{vis} = 0.3\) and \(S = 0.5\).

From: Hydrodynamic analysis of the magnetic field dependent viscous fluid flow and thermosolutal convection between rotating channels

m

\(f''(0)\)

\(-\,g'(0)\)

\(-\,h'(0)\)

\(-\,k'(0)\)

\(-\,\theta ' (0)\)

\(-\,\Psi ' (0)\)

1

3.30248492

0.76935826

\(-0.76249352\)

\(-0.86198432\)

1.01629436

1.00261843

6

3.30248445

0.76935839

\(-0.76249348\)

\(-0.861984256\)

1.01629429

1.00261862

12

3.30248472

0.76935856

\(-0.76249352\)

\(-0.861984261\)

1.01629435

1.00261869

18

3.30248472

0.76935856

\(-0.76249352\)

\(-0.861984261\)

1.01629435

1.00261869

24

3.30248472

0.76935856

\(-0.76249352\)

\(-0.861984261\)

1.01629435

1.00261869

30

3.30248472

0.76935856

\(-0.76249352\)

\(-0.861984261\)

1.01629435

1.00261869