1960
DOI: 10.1088/0370-1328/76/2/307
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Underwater Explosions as Acoustic Sources

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Cited by 90 publications
(47 citation statements)
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“…Taking a look at each term: 10 log 10 \×(j) 1 2 is the dB power level out of our spectrum program re 1 digital unit, or 1 µV, 10 log 10 C 2 (j) = 20 log 10 CU) is the dB response of the system re µV/ (cm/s), and 10 log 10 (poco2 f} = 10 log 10 [(2.3 g/cm 2 )(3 × 10 5 cm/s)(2)(20.48 s)] The energy-flux-density of the source, (10 log 10 E s ), must be calculated for each source used, or using the method of Weston (1960).…”
Section: U)mentioning
confidence: 99%
“…Taking a look at each term: 10 log 10 \×(j) 1 2 is the dB power level out of our spectrum program re 1 digital unit, or 1 µV, 10 log 10 C 2 (j) = 20 log 10 CU) is the dB response of the system re µV/ (cm/s), and 10 log 10 (poco2 f} = 10 log 10 [(2.3 g/cm 2 )(3 × 10 5 cm/s)(2)(20.48 s)] The energy-flux-density of the source, (10 log 10 E s ), must be calculated for each source used, or using the method of Weston (1960).…”
Section: U)mentioning
confidence: 99%
“…The acoustical properties of explosives are summarised by Weston (1960Weston ( , 1962. The main feature is a short shock wave comprising a sharpalmost instantaneous-rise in pressure followed by an exponential decay with a time constant of a few hundred microseconds.…”
Section: Pressure Measurements Of Large Explosions In Shallow Watermentioning
confidence: 99%
“…The main feature is a short shock wave comprising a sharpalmost instantaneous-rise in pressure followed by an exponential decay with a time constant of a few hundred microseconds. The expanding shock wave creates a large pulsating bubble with successive expansions and contractions that give rise to a series of weaker, more symmetrical bubble pulses as happens also with an airgun pulse (Weston, 1960;Cole, 1965). In shallow water, the multiple interactions of the shock and acoustic waves create a more complex pattern.…”
Section: Pressure Measurements Of Large Explosions In Shallow Watermentioning
confidence: 99%
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“…The advantages of short pulses as broad band sources with optimum time resolution have lead to the widespread employment of explosive charges, electric sparks, and other impulse generators such as the Edgerton Thumper or Boomer as sonic sources for hydroacoustic measurements (Weston, 1960;Worzel, Ewing, and Pekeris 1948;Hersey, Edgerton, Raymond, and Hayward 1960;Hoskins and Knott, 1961;Knott and Hersey, 1956). The extremely short rise time and exponential decay of at least some parts of the signal emitted by most of these sources lends itself to accurate analysis of very small travel time differences by the use of wide band filtering at medium to high frequencies.…”
mentioning
confidence: 99%