Table 3 Comparison of the SLLM results of $-f^{″}(0)$, $g^{\prime }(0)$, $-{\theta }^{\prime }(0)$ with those obtained by $bvp4c$ for different values of the Hall parameter

$\mathbf{-}{\mathit{f}}^{\mathbf{″}}\mathbf{(}\mathbf{0}\mathbf{)}$

${\mathit{g}}^{\mathbf{\prime }}\mathbf{(}\mathbf{0}\mathbf{)}$

$\mathbf{-}{\mathit{\theta }}^{\mathbf{\prime }}\mathbf{(}\mathbf{0}\mathbf{)}$