2016
DOI: 10.1016/j.jppr.2016.11.006
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Numerical investigation of two-dimensional and axisymmetric unsteady flow between parallel plates

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Cited by 7 publications
(6 citation statements)
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“…Assuming the above conditions, the time‐dependent leading equations are written in this way 6,28 : ux+vy=0, $\frac{\,\partial u}{\partial x}+\frac{\partial v}{\partial y}=0,$ ut+uux+vuy=1ρPx+ν2ux2+2uy2, $\frac{\partial u}{\partial t}+u\frac{\partial u}{\partial x}+v\frac{\partial u}{\partial y}=-\frac{1}{\rho }\frac{\partial P}{\partial x}+\nu \left(\frac{{\partial }^{2}u}{\partial {x}^{2}}+\frac{{\partial }^{2}u}{\partial {y}^{2}}\right),$ vt+uvx+vvy=1ρPy+ν2vx2+2vy2, $\frac{\partial v}{\partial t}+u\frac{\partial v}{\partial x}+v\frac{\partial v}{\partial y}=-\frac{1}{\rho }\frac{\partial P}{\partial y}+\nu \left(\frac{{\partial }^{2}v}{\partial {x}^{2}}+\frac{{\partial }^{2}v}{\partial {y}^{2}}\right),$ Tt+uTx+vTy=κρCp2Tx2+…”
Section: Mathematical Modelingmentioning
confidence: 99%
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“…Assuming the above conditions, the time‐dependent leading equations are written in this way 6,28 : ux+vy=0, $\frac{\,\partial u}{\partial x}+\frac{\partial v}{\partial y}=0,$ ut+uux+vuy=1ρPx+ν2ux2+2uy2, $\frac{\partial u}{\partial t}+u\frac{\partial u}{\partial x}+v\frac{\partial u}{\partial y}=-\frac{1}{\rho }\frac{\partial P}{\partial x}+\nu \left(\frac{{\partial }^{2}u}{\partial {x}^{2}}+\frac{{\partial }^{2}u}{\partial {y}^{2}}\right),$ vt+uvx+vvy=1ρPy+ν2vx2+2vy2, $\frac{\partial v}{\partial t}+u\frac{\partial v}{\partial x}+v\frac{\partial v}{\partial y}=-\frac{1}{\rho }\frac{\partial P}{\partial y}+\nu \left(\frac{{\partial }^{2}v}{\partial {x}^{2}}+\frac{{\partial }^{2}v}{\partial {y}^{2}}\right),$ Tt+uTx+vTy=κρCp2Tx2+…”
Section: Mathematical Modelingmentioning
confidence: 99%
“…As the symmetric nature of flow is considered, the associated boundary conditions are given by 6,42 u=Luy, v=vh=italicdhitalicdt, T=TH, C=CHaty=h(t), $u=-L\frac{\partial u}{\partial y},\unicode{x02007}v={v}_{h}=\frac{{dh}}{{dt}},\unicode{x02007}T={T}_{H},\unicode{x02007}C={C}_{H}\,\text{at}\,y=h(t),$ uy=Ty=Cy=0aty=0. $\frac{\partial u}{\partial y}=\frac{\partial T}{\partial y}=\frac{\partial C}{\partial y}=0\,\text{at}\,y=0.$…”
Section: Mathematical Modelingmentioning
confidence: 99%
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“…They also studied the problem in which lower plate rotates and upper plate stretches or shrinks. Raissi et al [17] studied the squeezing flow of viscous fluid under the effects of heat and mass transfer. Mohyud-Din and Khan [18] investigated the nonlinear radiation effects on the flow of a Casson fluid flowing through parallel discs with the lower disc taken to be permeable and the upper one solid.…”
mentioning
confidence: 99%