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A History of Research and a Review of Recent Developments

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Underwater explosions 51<br />

Figure 2.19 Measured <strong>and</strong> calculated radius <strong>of</strong> the gas sphere from a detonator one<br />

foot below the surface (from Herring, ref. 2.33).<br />

Since the total energy associated with the radial flow <strong>of</strong> water (Y) is given<br />

approximately by<br />

(2.19)<br />

it is possible to express the first oscillation period in terms <strong>of</strong> total energy by<br />

(2.20)<br />

This is a formula attributed to H.F.Willis, a British scientist, <strong>and</strong> shows that<br />

the period is directly proportional to the cube root <strong>of</strong> the explosive charge<br />

weight, since for most high explosive the total energy varies with charge weight.<br />

The period also varies as (d+33) –5/6 , where d is the water depth in feet, <strong>and</strong> this<br />

was verified experimentally by Ewing <strong>and</strong> Crary [2.32] who brought together<br />

the results <strong>of</strong> several studies to produce Figure 2.20. It was also shown that to<br />

a close approximation the periods <strong>of</strong> the first <strong>and</strong> second bubble oscillations<br />

are related by the formula<br />

(2.21)<br />

where T 1 <strong>and</strong> T 2 are the periods, <strong>and</strong> r 2 <strong>and</strong> r 1 are the fractional energies<br />

remaining after the first <strong>and</strong> second contractions.<br />

For depths greater than 320 feet T2/T 1 is very nearly constant <strong>and</strong> independent<br />

<strong>of</strong> depth, <strong>and</strong> is equal to about 0.6. This gives an energy ratio <strong>of</strong> 0.36.

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