Exact solution of the fundamental equation of acoustics for a pressure wave developing in two directions

V. Borodin, A. Lun-Fu, M. Bubenchikov, A. Bubenchikov, D. Mamontov
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Abstract

The authors proceed from the hyperbolic equation for acoustic pressure. Using the integral Fourier transform along the axial coordinate, an equation in partial derivatives for the kernel of this transformation is found. This equation contains only one spatial coordinate and time. Applying the integral Laplace transform in time to the last equation, we obtain an ordinary differential equation with respect to the radial coordinate for the corresponding image. It turns out that the solution of the last equation is the well-known Macdonald function. For this function, it was possible to find the original image according to Laplace. All this made it possible to write an integral formula for the pressure in a sound wave. If the function of the initial pressure distribution along the pipe axis is taken in the form of a Gaussian impulse, then the integrals included in the representation of the desired solution are taken explicitly. As a result, we obtain an explicit compact formula for the acoustic pressure distribution in the axisymmetric case. It is convenient to use this formula to analyze the distribution of sound disturbances both along the pipe axis and in the radial direction. Therefore, the results are presented as isobars in the (z, r) plane corresponding to different times.
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两个方向上压力波的声学基本方程的精确解
作者从声压的双曲方程出发。利用沿轴坐标的傅里叶积分变换,得到了该变换核函数的偏导数方程。这个方程只包含一个空间坐标和时间。对最后一个方程进行时间上的拉普拉斯积分变换,得到相应图像在径向坐标下的常微分方程。最后一个方程的解是著名的麦克唐纳函数。对于这个函数,可以根据拉普拉斯定理找到原始图像。所有这些使得写出声波压强的积分公式成为可能。如果将沿管道轴的初始压力分布的函数取为高斯脉冲的形式,则可以显式地取期望解的表示中包含的积分。得到了轴对称情况下声压分布的显式紧凑公式。利用该公式可以方便地分析沿管道轴向和径向的声扰动分布。因此,结果以(z, r)平面对应不同时间的等压线表示。
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0.90
自引率
66.70%
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