首页> 外文会议>AIAA/CEAS aeroacoustics conference >A new formulation of time domain boundary integral equation for acoustic wave scattering in the presence of a uniform mean flow
【24h】

A new formulation of time domain boundary integral equation for acoustic wave scattering in the presence of a uniform mean flow

机译:均匀平均流存在下声波散射时域边界积分方程的新公式

获取原文

摘要

It has been well-known that under the assumption of a constant uniform mean flow, the acoustic wave propagation equation can be formulated as a boundary integral equation, in both the time domain and the frequency domain. Compared with solving partial differential equations, numerical methods based on the boundary integral equation have the advantage of a reduced spatial dimension and, hence, requiring only a surface mesh. However, the constant uniform mean flow assumption, while convenient for formulating the integral equation, does not satisfy the solid wall boundary condition wherever the body surface is not aligned with the uniform mean flow. In this paper, we argue that the proper boundary condition for the acoustic wave is not that its normal velocity be zero everywhere on the solid surfaces, as has been applied in the literature. A careful study of the acoustic energy conservation equation is presented that shows such a boundary condition in fact leads to erroneous source or sink points on solid surfaces not aligned with the mean flow. A new solid wall boundary condition is proposed that conserves the acoustic energy and a new time domain boundary integral equation is derived. In addition to conserving the acoustic energy, another significant advantage of the new equation is that it is considerably simpler than previous formulations. In particular, tangential derivatives of the solution on the solid surfaces are no longer needed in the new formulation, which greatly simplifies numerical implementation. Furthermore, stabilization of the new integral equation by Burton-Miller type reformulation is presented. The stability of the new formulation is studied theoretically as well as numerically by an eigenvalue analysis. Numerical solutions are also presented that demonstrate the stability of the new formulation.
机译:众所周知,在恒定的平均流量恒定的假设下,声波传播方程可以在时域和频域中被公式化为边界积分方程。与求解偏微分方程相比,基于边界积分方程的数值方法具有减小空间尺寸的优势,因此仅需要表面网格即可。然而,恒定的均匀平均流量假设虽然便于公式化积分方程,但无论车身表面未与均匀平均流量对齐,都不能满足固体壁边界条件。在本文中,我们认为,声波的适当边界条件不是其在固体表面上各处的法向速度为零,正如文献中所应用的那样。仔细研究了声能守恒方程,结果表明,这种边界条件实际上会导致固体表面上与平均流不对齐的源或汇点出现错误。提出了一种新的节省声能的固壁边界条件,并推导了新的时域边界积分方程。除了节省声能之外,新方程式的另一个显着优点是,它比以前的公式要简单得多。特别是,在新的配方中不再需要溶液在固体表面上的切向导数,这大大简化了数值实现。此外,提出了通过Burton-Miller型重新公式化对新积分方程的稳定化。通过特征值分析对新配方的稳定性进行了理论和数值研究。还提出了数值解,证明了新配方的稳定性。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号