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中文核心期刊

用射线方法计算浅海混响平均强度(Ⅱ)

CALCULATION OF SHALLOW WATER REVERBERATION INTENSITY BASED ON RAY THEORY, PART (Ⅱ)

  • 摘要: 本文推广前文所述计算均匀层浅海远程混响强度的方法,使之能对由两个等速层L1(靠近海底)、L3(靠近海面)和一夹于其间的梯度层L2所构成的非均匀浅海进行计算。
    在这种混合层中的声线按其能否穿透梯度层L2可分为两类。考虑到在远程情况下所有有效声线的掠射角都较小,从而可近似地求得计算混响所需的各声线的掠射角。文中计算了收发合置于上层L3时的海底和海面混响强度I3b+I3b-I3s+,这里“±”表示梯度a(≥)0。远程的计算结果表明I3b+r-7/2(对均匀散射)、I3b+r-4(对兰贝特散射)、I3b-r-5(对两种散射),I3b+r-1(对均匀散射)。
    对收发合置于下层L1的情况可作类似的计算,不会遇到更多的困难。

     

    Abstract: The method used for calculating the long range reverberation intensity in shallow homogeneous layer had been described in part I. It will be extented to include the inhomogeneous layer consisted of two isovelocity layers L1 (near the bottom), L3(near the surface) and a gradient layer L2 (Located between L1 and L3) in this paper.
    The rays in this mixed layer may be divided into two classes according to whether they can penetrate through the gradient layer L2. Considering the faet that, at long ranges, the grazing angles of all effective rays would be small, thie grazing angles needed to caleulate the reverberation can be obtained approximately for both elasses. Then the bottom and the surface reverberation intensities I3b+I3b- and I3s+ are calculated analytically, as the projector and the receiver are at thle same place in layer Ls (the sign "+" or "-",means the velocity gradient a> >0 or a< 0).The results for adequate long range show that I3b+~r-7/2 (for the omnidirectional scattering),-r-4 (for the lambert's scattering),I3b-~r-5 (for both sciattering) and I3b+~r-1 (for the omnidirectional scattering).
    A similar caleulation can be carried out as well for the case the projector and the receiver are at the same place in L1, and no more difficulties will exist.

     

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