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UNSTEADY HEAT OR MASS TRANSPORT FROM A SUSPENDED PARTICLE AT LOW PECLET NUMBERS

机译:悬浮粒子以低Peclet数进行的非稳定传热或传质

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Unsteady heat or mass transport from a particle with an arbitrary shape suspended in a fluid of infinite expanse is considered in the limit of small Peclet numbers where diffusion is dominant. In a frame of reference in which the particle appears to be stationary, the velocity of the fluid is uniform or varies in a linear manner with respect to the spatial coordinates, with an arbitrary time dependence. The temperature or concentration of a species at the surface of the particle is held at a certain constant value, whereas that at infinity is held at another constant value. Two particular problems are considered, both to leading order with respect to the Peclet number: (a) the rate of transport from a particle that is introduced suddenly into a steady flow near the steady state; and (b) the average rate of transport from a particle that is suspended in a time-periodic flow. The theory uses the method of matched asymptotic expansions and employs the Green's function of the convection-diffusion equation for a generally unsteady uniform or linear flow. The Green's function is derived in closed form by first performing a transformation to a Lagrangian framework. In the first problem of transient transport, it is found that the functional form of the rate of transport near the steady state is affected strongly by the structure of the incident flow: the decay in uniform or elongational flow is exponential, whereas the decay in simple shear flow is algebraic. In the second problem of transport in a periodic flow, it is found that the value of a properly defined frequency parameter has a strong influence on the mean rate of transport, for all types of flow. The oscillation induces convective mixing and thereby reduces the mean rate of transport bq a substantial factor. The ability of the theory to describe another situation of heat or mass transport considered by Pedley is also discussed. [References: 29]
机译:悬浮在无限膨胀的流体中的任意形状的颗粒产生的不稳定或热传输被认为是小Peclet数的限制,其中扩散占主导地位。在其中粒子看起来是静止的参考系中,流体的速度相对于空间坐标是均匀的或以线性方式变化的,并且具有任意时间依赖性。粒子表面的物质的温度或浓度保持在某个恒定值,而无穷大的温度或浓度保持在另一个恒定值。考虑了两个特殊的问题,这两个问题相对于Peclet数都处于领先地位:(a)从突然引入到稳态附近的稳态流中的粒子的传输速率; (b)悬浮在时间周期流中的粒子的平均传输速率。该理论使用匹配渐近展开法,并采用对流扩散方程的格林函数来求解通常不稳定的均匀或线性流动。通过首先执行到拉格朗日框架的转换,以封闭形式派生格林函数。在第一个瞬态传输问题中,发现稳态附近传输速率的函数形式受入射流结构的强烈影响:均匀流或伸长流的衰减是指数的,而简单流的衰减是指数的剪切流是代数的。在周期性流动中的第二个运输问题中,发现对于所有类型的流动,适当定义的频率参数的值都对平均运输速率有很大的影响。振荡引起对流混合,从而大大降低了平均运输速率。还讨论了该理论描述佩德利所考虑的另一种传热或传质情况的能力。 [参考:29]

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