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中文核心期刊

WU Cheng-yi. CALCULATION OF SHALLOW WATER REVERBERATION INTENSITY BASED ON RAY THEORY, PART (Ⅱ)[J]. ACTA ACUSTICA, 1980, 5(3): 210-220. DOI: 10.15949/j.cnki.0371-0025.1980.03.007
Citation: WU Cheng-yi. CALCULATION OF SHALLOW WATER REVERBERATION INTENSITY BASED ON RAY THEORY, PART (Ⅱ)[J]. ACTA ACUSTICA, 1980, 5(3): 210-220. DOI: 10.15949/j.cnki.0371-0025.1980.03.007

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

  • 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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