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Oblique stagnation-point flow of an incompressible visco-elastic fluid towards a stretching surface

机译:不可压缩的粘弹性流体向拉伸表面的倾斜停滞点流动

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摘要

An analysis is made of the steady two-dimensional stagnation-point flow of an incompressible viscoelastic fluid over a flat deformable surface when the surface is stretched in its own plane with a velocity cx, where x is the distance from the stagnation-point and c is a positive constant. It is shown that for a viscoelastic fluid of short memory (obeying Walters' B model), a boundary layer is formed when the stretching velocity of the surface is less than ax, where ax + 2by is the inviscid free-stream velocity and y is the distance normal to the plate, a and b being constants and the velocity at a point increases with increase in the elasticity of the fluid. On the other hand an inverted boundary layer is formed when the surface stretching velocity exceeds ax and the velocity decreases with increase in the elasticity of the fluid. A novel result of the analysis is that the flow near the stretching surface is that corresponding to an inviscid stagnation-point flow when a = c. Temperature distribution in the boundary layer is found in three cases, namely: (ⅰ) the sheet with constant surface temperature (CST); (ⅱ) the sheet with variable surface temperature (VST) and (ⅲ) the sheet with prescribed quadratic power law surface heat flux (PHF) for various values of non-dimensional parameters. It is found that in all the three cases when a/c > 1, temperature at a point decreases with increase in the elasticity of the fluid and when a/c < 1, temperature at a point increases with increase in the elasticity of the fluid. Further temperature at a point decreases with increase in the radiation parameter and wall temperature parameter.
机译:分析了当不可压缩的粘弹性流体在其自身平面中以速度cx拉伸时,不可压缩粘弹性流体在平面可变形表面上的稳定二维停滞点流动,其中x是到停滞点的距离,c是一个正常数。结果表明,对于记忆短的粘弹性流体(服从Walters B模型),当表面的拉伸速度小于ax时会形成边界层,其中ax + 2by是无粘性的自由流速度,y是垂直于板的距离,a和b为常数,并且一点的速度随流体弹性的增加而增加。另一方面,当表面拉伸速度超过ax且速度随着流体的弹性增加而降低时,会形成一个倒置的边界层。该分析的新颖结果是,在拉伸表面附近的流动是当a = c时对应于不粘滞点的流动。边界层中的温度分布有以下三种情况:(ⅰ)具有恒定表面温度(CST)的薄板; (ⅱ)表面温度(VST)可变的薄片,(ⅲ)具有规定的二次幂律表面热通量(PHF)的薄片,用于各种非尺寸参数值。发现在所有三种情况下,当a / c> 1时,点的温度随着流体的弹性增加而降低;当a / c <1时,点的温度随着流体的弹性增加而增加。 。随着辐射参数和壁温度参数的增加,某一点的进一步温度降低。

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