Descriptive Summary of the Theory of Sound Scattering By Rods Rings Grids And

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Descriptive Summary of the Theory of Sound Scattering By Rods Rings Grids And
J K L Macdonald
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Il'or thia or^linJora (or srall 3jher0a» or in geaera^ for thin rode and lumpa) tl ie ^reverse ia the eaao (tho pressure aaplitudes being hardly altered in the region occupied by tha aylinder* but nagniflcatiam of the rate of ehange of presatira idtt diatanaa outward near tha eylinder being laroduoed in tha ratio of "aolid danaity to water denaity". ) Pw a perfeotly i-erieotlng half plane tl'^o amplitudaa ai'e unalteroJ uo the ed^ vflien the refleetor ia introduced . Hoarever, within about thre...e wavelengtha from the ed^ the applitudoa are alrraoat doubiod on tlio "exposed" nido o^' ttie refleotor« and are reduced almoat to eero on the "ahaded aide". Sinoe Htm - 4 - mtrelength of sound used Is about 6 «n as contrasted vrifh around 0. 00006 em for light« acoustio sliadow effects are relatively diffuse.
The different obaraoterlstic changes in tho local asplitudes when thin shells « thin rods and large reflecting shields are placed in the path of sound waves correspond to the production of different eharaoteristio secondary source distri- butions.


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