By Lewis Larmore (auth.), A. F. Metherell, Lewis Larmore (eds.)

This quantity offers the complaints of the second one foreign Sym posium on Acoustical Holography, which was once held on the Douglas complex learn Laboratories on 6 and seven March 1969, fifteen months after the 1st symposium. area used to be constrained to approximately a hundred and ten seats, with representatives from 9 nations attending. those nations incorporated Canada, England, France, Japan, Mexico, Scotland, Sweden, Switzerland, and the USA. The symposium consisted of 21 formal papers. The 22nd, through Dr. U. Fehr, was once now not learn, yet is incorporated in those court cases. The manu script of the attention-grabbing paper on acoustic propagation in a turbulent medium which used to be learn by means of Dr. O. okay. Mawardi was once now not got in time for e-book in those complaints, and we glance ahead to its book might be at a later date within the open literature. as well as the formal papers there have been 3 casual displays on the finish of the assembly that have been given through Dr. A. Lohmann, by way of L. A. Cram and okay. O. Rossiter, and by means of T. S. Graham, that are additionally integrated in those court cases. on the finish of the formal displays Dr. Lewis Larmore summarized the symposium and mentioned a few of the highlights. For the symposium precis and a precis of those lawsuits the reader is pointed out bankruptcy 1.

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Korpel 48 According to the theory of stationary phase,7 the solution of (27) is then given by for 02A(S)}-1/2 III/~(s)1 = - 1m [ (2n)1/2 { ~ Sa S < Sa (35) { n}] g(Sa) exp jA(sa) + j4 for S > Sa We will assume that the phase of the generated ray is such that its amplitude is a maximum. E(Sa)1 (2n)1/2{ O~~~S) (37) r 1/2, (38) Hence, the amplitude of the Hertz vector equals zero before the ray meets the surface ~. Upon crossing the surface, it acquires a value given by (38) with phase given by (37).

The Equation of the Pseudoray The foundation of the desired expression for the pseudoray was developed in the previous sections. We begin by combining Eqs. (r) e ikt/J L. - - -_ e ikt/Jao (ik)' (1 + a , + . ,) 1 iaok (49) Osman K. () r, t 'f' 1 2n = - Ix; aoexp - i{wt - [kl/l - (at/aok) w - Wo -00 + ... J} dw + I (50) where I stands for the contribution of the scattered signal. If it is assumed for the sake of simplicity that no scattering takes place in the path of the propagating signal, then the dependence of k on the frequency is given by k = w/c (51) where the velocity of propagation c is a function of position.

But from the Hamilton-Jacobi relation (15), the front of the wave F in configuration space advances like (W - Et). If W is made to correspond to f, then, by symmetry, the energy E must be proportional to the frequency. This is of course the quantum condition E = nw (16) A puzzling point which appears in classical mechanics is the interpretation of the velocity with which the wavefront of F propagates. This velocity is readily computed as follows. , along a ray. But from (11), L1 W = E L1t. Hence, if we denote this velocity of propagation by u, then (18) u = ds/dt and, using the above result, u = E/IVWI (19) Combining (19) with (15), it immediately follows that u = E/[2m(E - V)P/2 (20) 28 Osman K.