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DETERMINISTIC AND DIFFUSIVE MASS TRANSFER MECHANISMS IN THE CAPTURE OF VAPORS AND PARTICLES.

机译:蒸气和颗粒捕获中确定性和扩散性的物质转移机制。

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摘要

Several analytical methods, some classical and some new, are employed to study the motion of dilute mixtures of particles or heavy molecules in a host gas. In the (particle) limit of negligible Brownian diffusivity, Robinson's extension of the potential flow theory to dust-laden fluids is re-introduced and more fully exploited. The generally overlooked but important phenomenon of particle phase compressibility is illustrated. It is shown that particle "inertial drift" and "pressure diffusion" are equivalent phenomena for host fluid deceleration times, (omega)('-1), which are large compared with the particle relaxation ("stopping") time (tau). Generalized phenomenological expressions, giving the particle velocity drift as a function of local fluid properties only (but valid for a much larger region of (omega)(tau) than the Chapman-Enskog expansion) are found. Although these phenomenological laws have been rigorously derived only for linear flows (in which the velocity field depends linearly on the spatial coordinates), it appears that the assumption of locally linear behavior leads to a valuable approximate description of the effects of inertia in particle motion even when the host fluid flow is not linear in the above sense. A useful analytical solution to the problem of the large Reynolds number motion of a dusty gas near the forward stagnation point of a cylinder in crossflow is derived, including inertial, diffusive (thermal and Brownian) and centrifugal effects. The analogous problem of a sphere in a low Reynolds number flow is also solved in the absence of thermophoresis. The generalized phenomenological laws obtained in the particle limit are extended to the case of non-negligible Fick diffusivity (heavy molecule limit) with the help of a Fokker-Planck kinetic equation.;Owing to its great practical interest, we conclude with a treatment of the thermophoretic deposition of particles in turbulent boundary layer flow. Available, but limited, experimental data have been used to test our predictions, and the agreement is found to be generally good.
机译:几种分析方法(一些经典方法和一些新方法)被用于研究基质气体中颗粒或重分子的稀混合物的运动。在可忽略的布朗扩散率的(粒子)极限中,罗宾逊将势流理论扩展到含尘流体的方法被重新引入并得到更充分的利用。说明了颗粒相可压缩性通常被忽视但很重要的现象。结果表明,粒子“惯性漂移”和“压力扩散”是主流体减速时间ω('-1)的等效现象,与粒子弛豫(“停止”)时间(tau)相比,这是很大的。发现了广义的现象学表达式,仅给出了随局部流体特性变化的粒子速度漂移(但对于比Chapman-Enskog扩展大得多的τ区域有效)。尽管仅对线性流严格地推导了这些现象学定律(其中速度场线性地依赖于空间坐标),但是看来局部线性行为的假设甚至可以对质点运动中的惯性效应做出有价值的近似描述。在上述意义上,当主流体流动不是线性的。得出了一种有用的分析解决方案,该解决方案包括在惯性,扩散(热和布朗)效应和离心效应下,在横流中靠近气缸前停滞点的尘埃气体大雷诺数运动的问题。在没有热泳的情况下,也解决了低雷诺数流中球体的类似问题。借助Fokker-Planck动力学方程,在粒子极限中获得的广义现象学定律扩展到不可忽略的Fick扩散率(重分子极限)的情况。湍流边界层流中颗粒的热泳沉积。可用的但有限的实验数据已用于检验我们的预测,并且发现该协议通常是好的。

著录项

  • 作者

    FERNANDEZ DE LA MORA, JUAN.;

  • 作者单位

    Yale University.;

  • 授予单位 Yale University.;
  • 学科 Plasma physics.
  • 学位 Ph.D.
  • 年度 1980
  • 页码 233 p.
  • 总页数 233
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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