2020
DOI: 10.1002/htj.22043
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A two‐component modeling for free stream velocity in magnetohydrodynamic nanofluid flow with radiation and chemical reaction over a stretching cylinder

Abstract: This analysis explores the influence of magnetohydrodynamic (MHD) nanofluid flow over a stretching cylinder with radiation effect in presence of chemically reactive species. The thermal radiation phenomenon is incorporated in the temperature equation. The mathematical modeling of the physical problem produces nonlinear set of partial differential equations corresponding to the momentum and energy equations that can be transformed into simultaneous system of ordinary differential equations with appropriate boun… Show more

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Cited by 14 publications
(9 citation statements)
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References 28 publications
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“…The governing equations are 2,47,49,50 (ru)x+(rv)r=0, $\frac{\partial (ru)}{\partial x}+\frac{\partial (rv)}{\partial r}=0,$ uux+vur=v)(2ur2+1rurσB02ρ(uU)+UUx, $u\frac{\partial u}{\partial x}+v\frac{\partial u}{\partial r}=v\left(\frac{{\partial }^{2}u}{\partial {r}^{2}}+\frac{1}{r}\frac{\partial u}{\partial r}\right)-\frac{\sigma {B}_{0}^{2}}{\rho }(u-{U}_{\infty })+{U}_{\infty }\frac{\partial {U}_{\infty }}{\partial x},$ uTx+vTr=α)(2Tr2+1rTr+τ][DBCyTy+false(DT/Tfalse)Ty21(ρc)f1rrfalse(rqrfalse), $u\frac{\partial T}{\partial x}+v\frac{\partial T}{\partial r}=\alpha \left(\frac{{\partial }^{2}T}{\partial {r}^{2}}+\frac{1}{r}\frac{\partial T}{\partial r}\right)+\tau \left[{D}_{B}\frac{\par...…”
Section: Mathematical Formulationmentioning
confidence: 99%
See 1 more Smart Citation
“…The governing equations are 2,47,49,50 (ru)x+(rv)r=0, $\frac{\partial (ru)}{\partial x}+\frac{\partial (rv)}{\partial r}=0,$ uux+vur=v)(2ur2+1rurσB02ρ(uU)+UUx, $u\frac{\partial u}{\partial x}+v\frac{\partial u}{\partial r}=v\left(\frac{{\partial }^{2}u}{\partial {r}^{2}}+\frac{1}{r}\frac{\partial u}{\partial r}\right)-\frac{\sigma {B}_{0}^{2}}{\rho }(u-{U}_{\infty })+{U}_{\infty }\frac{\partial {U}_{\infty }}{\partial x},$ uTx+vTr=α)(2Tr2+1rTr+τ][DBCyTy+false(DT/Tfalse)Ty21(ρc)f1rrfalse(rqrfalse), $u\frac{\partial T}{\partial x}+v\frac{\partial T}{\partial r}=\alpha \left(\frac{{\partial }^{2}T}{\partial {r}^{2}}+\frac{1}{r}\frac{\partial T}{\partial r}\right)+\tau \left[{D}_{B}\frac{\par...…”
Section: Mathematical Formulationmentioning
confidence: 99%
“…Ismail et al 43 analyzed heat transfer and suction due to the MHD flow of copper and alumina nanofluids past a porous stretching surface under the influence of nonlinear radiation effects. Over different boundary conditions, nanofluids are more demandable in the presence of non‐Newtonian fluids 44–48 …”
Section: Introductionmentioning
confidence: 99%
“…Poply and Vinita 10 considered radiation and heat generation effects in their heat transfer analysis of nanofluid over stretching cylinder. Vinita et al 11 presented the two-components modeling of free stream velocity for MHD nanofluids over stretching cylinder. Jamshed et al 12 – 14 presented an optimal case study for evaluating unsteady nanofluid along a stretching surface, a mathematical model for heat transfer analysis of second grade nanofluid over a permeable flat surface, also done a comparative study of Williamson nanofluid by using Keller box method.…”
Section: Introductionmentioning
confidence: 99%
“…Vinita et al [10] explained the effect of variable slip flows in addition to thermal radiation in MHD nanofluids induced by non linear stretched surface. Vinita et al [11] examined radiation effect on MHD free stream velocity nanofluid flow induced by stretchable cylinder in presence of chemically reactive species by applying RKF technique using ODE45 solver in MATLAB. Khan et al [12] studied the applications of bio-convection nanofluid flow in presence of activation energy.…”
Section: Introductionmentioning
confidence: 99%