Descriptive Summary of the Theory of Sound Scattering By Rods Rings Grids And
Descriptive Summary of the Theory of Sound Scattering By Rods Rings Grids And
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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.
What to read after Descriptive Summary of the Theory of Sound Scattering By Rods Rings Grids And?
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To quickly assess the difficulty of the text, read a short excerpt:
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.
What to read after Descriptive Summary of the Theory of Sound Scattering By Rods Rings Grids And?
You can find similar books in the "Read Also" column, or choose other free books by J K L Macdonald to read onlineMoreLess
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