2020
DOI: 10.1002/htj.22011
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Mixed convection flows of tangent hyperbolic fluid past an isothermal wedge with entropy: A mathematical study

Abstract: The nonlinear, steady, and mixed convective boundary layer flow and heat transfer of an incompressible tangent hyperbolic non‐Newtonian fluid over an isothermal wedge in the presence of magnetic field are analyzed numerically using the implicit Keller‐Box finite‐difference technique. The entropy analysis due to MHD flow of a tangent hyperbolic fluid past an isothermal wedge and viscous dissipation is also included. The numerical code is validated with previous Newtonian studies available in the literature. Gra… Show more

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Cited by 13 publications
(4 citation statements)
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“…The flow is subjected to a porous medium and a constant magnetic field intensity B = B 0 which is considered perpendicular to the wedge surface while the wedge surface is taken in the x ‐direction. The fluid flow equations over a stretching wedge expressed as 3,38–43 : ux+vy=0, $\frac{\partial u}{\partial x}+\frac{\partial v}{\partial y}=0,$ uux+vuy=UdUdx+υ2uy2σ*B02ρf(uU)υκ1(uU)+1ρf[ρfgβT(TT)(ρpρf)gβC(trueC¯C¯)]sinΩ2, $u\frac{\partial u}{\partial x}+v\frac{\partial u}{\partial y}=U\frac{dU}{dx}+\upsilon \frac{{\partial }^{2}u}{\partial {y}^{2}}-\frac{\sigma * {B}_{0}^{2}}{{\rho }_{f}}(u-U)-\frac{\upsilon }{{\kappa }_{1}}(u-U)+\frac{1}{{\rho }_{f}}[{\rho }_{f}g{\beta }_{T}(T-{T}_{\infty })-({\rho }_{p}-{\rho }_{f\infty })g{\beta }_{C}(\bar{C}-{\bar{C}}_{\infty })]\sin \left(\frac{\Omega }{2}\right),$ uTx+vTy=μcp][UdUdx+σ*B02U+αf+16σsT33k*(...…”
Section: Governing Equationsmentioning
confidence: 99%
See 1 more Smart Citation
“…The flow is subjected to a porous medium and a constant magnetic field intensity B = B 0 which is considered perpendicular to the wedge surface while the wedge surface is taken in the x ‐direction. The fluid flow equations over a stretching wedge expressed as 3,38–43 : ux+vy=0, $\frac{\partial u}{\partial x}+\frac{\partial v}{\partial y}=0,$ uux+vuy=UdUdx+υ2uy2σ*B02ρf(uU)υκ1(uU)+1ρf[ρfgβT(TT)(ρpρf)gβC(trueC¯C¯)]sinΩ2, $u\frac{\partial u}{\partial x}+v\frac{\partial u}{\partial y}=U\frac{dU}{dx}+\upsilon \frac{{\partial }^{2}u}{\partial {y}^{2}}-\frac{\sigma * {B}_{0}^{2}}{{\rho }_{f}}(u-U)-\frac{\upsilon }{{\kappa }_{1}}(u-U)+\frac{1}{{\rho }_{f}}[{\rho }_{f}g{\beta }_{T}(T-{T}_{\infty })-({\rho }_{p}-{\rho }_{f\infty })g{\beta }_{C}(\bar{C}-{\bar{C}}_{\infty })]\sin \left(\frac{\Omega }{2}\right),$ uTx+vTy=μcp][UdUdx+σ*B02U+αf+16σsT33k*(...…”
Section: Governing Equationsmentioning
confidence: 99%
“…Rashidi et al 2 addressed non‐Newtonian fluid flow over a nonisothermal wedge using homotopy analysis. Ramesh Reddy et al 3 examined the implicit‐based mixed convective flow of non‐Newtonian hyperbolic tangent fluid flow over an isothermal wedge. Multiple slip effects are examined with chemically reactive magneto‐Carreau fluid flow over a wedge is addressed by Khan and Hashim 4 .…”
Section: Introductionmentioning
confidence: 99%
“…Because creep resistance is present and it has high shear viscosity, it is classified as a shear-thinning fluid. After the shear stress exceeds the elastic limit, it behaves in a similar manner as a Newtonian fluid, as shown by Reddy et al [6]. Retardation and relaxation times in the Jeffrey fluid model are important for denoting the viscoelastic properties of polymeric materials, as shown by Bajwa et al [7].…”
Section: Introductionmentioning
confidence: 77%
“…Madhavi et al 3 analyzed the entropy analysis of MHD convection flow from a flat cylinder with slip. Ramesh Reddy et al 4 studied the entropy of mixed convection flows of tangent hyperbolic fluid across an isothermal wedge. Beg and Makinde 5 researched the Maxwell fluid flow and mass transfer in a Darcian porous channel.…”
Section: Introductionmentioning
confidence: 99%