2018
DOI: 10.1166/jon.2018.1474
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Slip Effects on Magneto Hydro Dynamic Stagnation Point Flow of Carreau-Nanofluid Over a Linear Sheet

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“…The exact solution of nonlinear coupled ordinary differential equations , , and is not possible. To facilitate the numerical solution of these equations, an implicit finite difference method, which is used by many researchers to investigate the solution of boundary value problems, is used. First of all, we reduce the higher‐order differential equation to the systems of first‐order differential equations, and the corresponding first‐order system is: ffalse′=p, pfalse′=q, qfalse′p2+fq+1=0, hfalse′=r, rfalse′+frph+false(αβfalse)=0, θfalse′=s, ϕfalse′=z, 1Prsfalse′+43PrRdfalse(1+false(θw1false)θfalse)3sfalse′+4PrRdfalse(θw1false)false(1+false(θw1false)θfalse)2s2+Du.25emz'+fs=0, z+ScSrs+ScfzScβϕn=<...>…”
Section: Solution Proceduresmentioning
confidence: 99%
“…The exact solution of nonlinear coupled ordinary differential equations , , and is not possible. To facilitate the numerical solution of these equations, an implicit finite difference method, which is used by many researchers to investigate the solution of boundary value problems, is used. First of all, we reduce the higher‐order differential equation to the systems of first‐order differential equations, and the corresponding first‐order system is: ffalse′=p, pfalse′=q, qfalse′p2+fq+1=0, hfalse′=r, rfalse′+frph+false(αβfalse)=0, θfalse′=s, ϕfalse′=z, 1Prsfalse′+43PrRdfalse(1+false(θw1false)θfalse)3sfalse′+4PrRdfalse(θw1false)false(1+false(θw1false)θfalse)2s2+Du.25emz'+fs=0, z+ScSrs+ScfzScβϕn=<...>…”
Section: Solution Proceduresmentioning
confidence: 99%