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Approximate formulae for the average one sided specific radiation wave impedance of a finite rectangular panel

机译:有限矩形面板的平均单侧比辐射波阻抗的近似公式

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The authors have previously published approximate formulae for the average one sided specific radiation wave impedance of a finite rectangular panel mounted in a rigid infinite baffle. The panel's transverse vibration was due to a (possibly forced) two dimensional bending plane wave propagating in the panel without reflection at the edges of the panel. The average was over all the surface area of the panel and over all possible azimuthal angles of propagation direction. The radiation from waves propagating in different directions was assumed to be uncorrelated. These approximate formulae were derived from the 1982 research of Thomasson whose approximate formulae only covered the high and low frequency regions and not the mid frequency region. This paper presents more accurate versions of some of the approximate formulae. When the bending wave number is larger than the wave number of sound, the real part of the impedance is smaller than that for the case studied by Maidanik and Leppington. This is because correlated reflections are not included the case analyzed in this paper. When the bending wave number is smaller than or equals the wave number of sound, the real part of the impedance is the same for both cases.
机译:作者先前已经发布了安装在刚性无限挡板中的有限矩形面板的平均单侧比辐射波阻抗的近似公式。面板的横向振动是由于(可能是受力的)二维弯曲平面波在面板中传播而在面板边缘没有反射所致。该平均值在面板的所有表面积上以及在传播方向的所有可能的方位角上。假定来自在不同方向传播的波的辐射是不相关的。这些近似公式来自1982年Thomasson的研究,该研究的近似公式仅覆盖高低频区域,而没有覆盖中频区域。本文介绍了一些近似公式的更准确的版本。当弯曲波数大于声音的波数时,阻抗的实部小于Maidanik和Leppington研究的情况。这是因为在本文分析的情况下不包括相关反射。当弯曲波数小于或等于声音的波数时,两种情况下阻抗的实部都相同。

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