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Torques on Solid Boundaries Caused by Inviscid Laminar Flows

机译:层流不粘稠导致的固体边界上的扭矩

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Certain homogeneous laminar fluid flows are examined for their time rates of change in orbital angular momentum in order to try to learn about the torques exerted by the fluid on nearby solid boundaries. A time rate of change in the angular momentum of the fluid must be caused by a torque induced in the fluid by the boundary as the fluid moves past it. Conversely, by an extension of Newton 's third law to rotary motion the fluid causes an equal but opposite torque on the boundary about the same axis. Friction is assumed negligible and the moving fluid is taken to be a two-dimensional shear flow without any vortices. First we consider the flow past a thin circular arc bump on an otherwise flat wall. Computing the angular momentum per unit volume about the center of the circular arc gives a time rate of increase in the angular momentum at the front half of the arc (encountered first by the flow), followed by a time rate of decrease at the back half. As a consequence of action equals reaction, the torque per unit volume imparted by the fluid to the front half of the arc tries to rotate it counterclockwise, while the torque on the back half tries to rotate it clockwise. There is no net torque on the arc. In magnitude the torques per unit volume on the arc are proportional to the fluid density and to the square of the mean speed of the fluid, and they increase with increasing thickness for constant horizontal length of the arc. Second, an example of flow past an asymmetrical bump is discussed in which it is argued that there is a net torque on the bump whose magnitude and direction are independent of the mean direction of flow. The sense of the net torque is to rotate the side of the bump with the lesser surface curvature toward the side with the greater surface curvature. Finally, the solitary wave is predicted to cause torques on a completely flat bottom as it passes by. Forces induced on solid boundaries that are directed parallel to the mean flow are mentioned.
机译:检查某些均匀的层状流体流的轨道角动量的时间变化率,以便尝试了解流体在附近的固体边界上施加的扭矩。流体的角动量的时间变化率必须由流体在运动通过边界时由边界在流体中感应出的扭矩引起。相反,通过将牛顿第三定律扩展到旋转运动,流体在绕同一轴的边界上产生相等但相反的转矩。假定摩擦微不足道,并且将运动流体视为二维剪切流而没有任何涡旋。首先,我们考虑流过原本平坦的壁上的薄圆弧形凸块的流动。计算绕圆弧中心的每单位体积的角动量会得出弧形前半部分的角动量按时间增加的速率(首先是由流动引起的),然后是后半部分的减小的时间率。由于作用等于反作用,流体施加到圆弧的前半部的每单位体积的扭矩会尝试使它逆时针旋转,而后半部的扭矩会尝试使其顺时针旋转。弧上没有净转矩。在大小上,电弧上每单位体积的转矩与流体密度和流体平均速度的平方成比例,并且对于恒定的电弧水平长度,它们随着厚度的增加而增加。其次,讨论了通过非对称凸块的流动的一个例子,其中认为在凸块上有一个净转矩,其大小和方向与平均流动方向无关。净转矩的含义是使表面曲率较小的凸块一侧向表面曲率较大的一侧旋转。最后,预计孤波在通过时会在完全平坦的底部上产生扭矩。提到了在平行于平均流的实心边界上引起的力。

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