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Acoustic/steady streaming from a motionless boundary and related phenomena: generalized treatment of the inner streaming and examples

机译:来自静止边界和相关现象的声音/稳定流:内部流的一般处理和示例

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摘要

As originally realized by Nyborg (J. Acoust. Soc. Am. vol. 30, 1958, p. 329), the problem of the inner acoustic/steady streaming can be analyzed in quite general terms. The inner streaming is the one that develops in the high-frequency limit in a thin Stokes (shear-wave) layer at a boundary, in contrast to the outer streaming in the main bulk of the fluid. The analysis provides relevant inner-streaming characteristics through a given distribution of the acoustic amplitude along the boundary. Here such a generalized treatment is revisited for a motionless boundary. By working in terms of surface vectors, though in elementary notations, new compact and easy-to use expressions are obtained. The most important ones are those for the effective (apparent) slip velocity at the boundary as seen from a perspective of the main bulk of the fluid, which is often the sole driving factor behind the outer streaming, and for the induced (acoustic) steady tangential stress on the boundary. As another novel development, non-adiabatic effects in the Stokes layer are taken into account, which become apparent through the fluctuating density and viscosity perturbations, and whose contribution into the streaming is often ignored in the literature. Some important particular cases, such as the axisymmetric case and the incompressible case, are emphasized. As far as the application of the derived general inner-streaming expressions is concerned, a few examples provided here involve a plane acoustic standing wave, which either grazes a wall parallel to its direction (convenient for the estimation of the non-adiabatic effects), or into which a small (compared to the acoustic wavelength) rigid sphere is placed. If there are simultaneously two such waves, out-of-phase and, say, in mutually orthogonal directions, a disk placed coplanarly with them will undergo a steady torque, which is calculated here as another example. Two further examples deal with translational high-frequency harmonic vibrations of particles relative to an incompressible fluid medium, viz. of a rigid oblate spheroid (along its axis) and of a sphere (arbitrary three dimensional). The latter can be a fixed rigid sphere, one free to rotate or even a (viscous) spherical drop, for which the outer streaming and the internal circulation are also considered.
机译:最初由尼堡(J. Acoust。Soc。Am。vol。30,1958,p。329)实现,内部声学/稳定流传输的问题可以用相当笼统的术语来分析。与流体的主要部分中的外部流相反,内部流是在边界处的薄斯托克斯(剪切波)层中在高频极限中发展的。该分析通过沿边界的给定声振幅分布提供了相关的内部流特征。在这里重新讨论了针对不动边界的这种广义处理。通过在表面向量方面进行操作,尽管使用基本符号,但可以获得新的紧凑且易于使用的表达式。最重要的是那些对于流体边界处的有效(表观)滑移速度(从流体的主要体积来看)的流体,这通常是外部流动背后的唯一驱动因素,而对于感生的(声波)则是稳定的。边界上的切向应力。作为另一个新颖的发展,考虑了斯托克斯层中的非绝热效应,这通过波动的密度和粘度扰动而变得明显,并且其对流的贡献在文献中常常被忽略。强调了一些重要的特殊情况,例如轴对称情况和不可压缩情况。就所推导的一般内部流表达式的应用而言,此处提供的一些示例涉及平面声驻波,该声驻波要么掠过平行于其方向的墙(便于估计非绝热效果),或在其中放入一个小的(与声波波长相比)刚性球体。如果同时存在两个这样的波,它们是异相的,并且例如在相互正交的方向上,则与它们共面放置的圆盘将承受稳定的扭矩,在此作为另一个示例进行计算。另外两个例子涉及粒子相对于不可压缩流体介质的平移高频谐波振动。刚性扁球体(沿其轴线)和球体(任意三维)的形状。后者可以是一个固定的刚性球体,可以自由旋转,甚至可以是(粘性)球形滴,为此还应考虑外部流动和内部循环。

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