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Brownian motion and thermophoresis effects on unsteady stagnation point flow of Eyring-Powell nanofluid: a Galerkin approach
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Z H Khan,M Usman,T Zubair,M Hamid,R U Haq
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Table 1. Comparison of the results achieved from the Galerkin method for $f^{\prime\prime} \left(0\right)$ and $\theta ^{\prime} \left(0\right)$ in the case of assisting flow when ${\rm{\Lambda }}=Nt=Nb=M=A={\lambda }_{f}=R={\lambda }_{\theta }=0$ and for various values of the Prandtl number.
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| [16] | [17] | Galerkin approach |
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Pr | $f^{\prime\prime} \left(0\right)$ $\theta ^{\prime} \left(0\right)$ | $f^{\prime\prime} \left(0\right)$ $\theta ^{\prime} \left(0\right)$ | $f^{\prime\prime} \left(0\right)$ $\theta ^{\prime} \left(0\right)$ |
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0.72 | 0.3645 | 1.0931 | 0.364 49 | 1.093 31 | 0.364 49 | 1.093 11 | 6.8 | 0.1804 | 3.2902 | 0.180 42 | 3.289 57 | 0.180 42 | 3.289 57 | 20 | 0.1175 | 5.6230 | 0.117 50 | 5.620 14 | 0.117 50 | 5.620 14 | 40 | 0.0873 | 7.9463 | 0.087 24 | 7.938 31 | 0.087 24 | 7.938 32 | 60 | 0.0729 | 9.7327 | 0.072 84 | 9.718 01 | 0.072 84 | 9.717 99 | 80 | 0.0640 | 11.2413 | 0.063 94 | 11.218 75 | 0.063 94 | 11.218 76 | 100 | 0.0578 | 12.5726 | 0.057 73 | 12.541 13 | 0.057 73 | 12.541 15 |
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