攻角、漂移角和偏航角速度联合作用下公转体的水动力和力矩计算

Y. Hong
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引用次数: 1

摘要

准确地预测潜航器船体和附属物上的水动力和力矩是确定其稳定性、控制和机动特性的必要条件。各种各样的分析方法已经被开发出来进行这些预测,包括计算流体力学的方法,但是没有一个是完全成功的。这是因为准确地确定船体表面上的速度分布和分隔线的位置是特别困难的。分离线的位置对作用在船体上的水动力和力矩的大小有重要的影响。本方法是参考文献1中讨论的技术的扩展。假定总水动力和力矩可分为无粘和粘两部分。用三维位势理论计算了力和力矩的非粘性部分。将物体表面离散为多个面元,并假设每个面元处的未知源和汇强度为常数。计算了表面单元处的速度,并将其保存下来,以便以后计算粘性力和力矩。应用层流和紊流的边界层理论计算了力和力矩的粘性部分。轴向力采用Young(2)提出的方法计算,横向力及其弯矩在二维横流存在分离的假设下计算。将边界层方程求解到分离点,并将摩擦阻力积分计算摩擦力。此外,假定在分离点以外的二维截面上有恒定的压力作用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Computation of the Hydrodynamic Forces and Moments Developed on a Body of Revolution at Combined Angles of Attack and Angles of Drift and Yawing Angular Velocities
The accurate prediction of the hydrodynamic forces and moments developed on the hull and appendages of a submerged vehicle is required for determining its stability, control, and maneuvering characteristics. Various analytical methods have been developed to make these predictions, including those of computational fluid dynamics, but none of them have been totally successful. This is because it is particularly difficult to accurately determine both the distribution of the velocity over the surface of the hull and the location of the separation lines. The location of the lines of separation has an important effect on the magnitude of the hydrodynamic forces and moments developed on the hull. The present method is an extension of the technique discussed in Reference 1. It is assumed that the total hydrodynamic force and moment can be divided into inviscid and viscous parts. The inviscid part of the forces and moments is computed using three dimensional potential theory. The body surface is discretized with many surface elements and the unknown strengths of the source and sink at each surface element are assumed to be constant. The velocities at surface elements are computed and saved for later computation of the viscous forces and moments. The viscous part of the forces and moments is computed with the application of the boundary layer theory for laminar and turbulent flows. The axial force is computed with the method of developed by Young (2). The lateral forces and its moments are computed under the assumption that there is separation in the two-dimensional cross flow. The boundary layer equation is solved to the separation point and the frictional drag is integrated to compute frictional force. Furthermore, it is assumed that a constant pressure is acting on the two dimensional section beyond the separation point.
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