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A History of Research and a Review of Recent Developments

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The decay <strong>of</strong> instantaneous overpressure in free air 21<br />

compare p 0 <strong>and</strong> R, that led to Eq. (1.9), she also measured positive phase<br />

durations, <strong>and</strong> from these results proposed the relationship<br />

(1.24)<br />

where z=R/W 1/3 in ft/lb 1/3 , t 0 is measured in milliseconds, <strong>and</strong> typical values <strong>of</strong><br />

c 1, <strong>and</strong> d 1, are:<br />

4000 lb bomb, high capacity, c1=8.1, d1=4.8 1000 lb bomb, medium capacity, c1=6.9, d1=4.2 1000 lb bomb, general purpose, c1=6.2, d1=3.8 As Figure 1.9 shows, the scatter is small. Similar curves to Figure 1.9, but for<br />

nuclear explosions were given in many publications in the 1950s.<br />

A knowledge <strong>of</strong> the instantaneous pressure <strong>and</strong> the duration <strong>of</strong> the positive<br />

phase allows us to calculate the blast impulse <strong>of</strong> an explosion. This is usually<br />

expressed per unit <strong>of</strong> projected area, <strong>and</strong> in imperial units is lb sec/in 2 or lb<br />

msec/in 2 . For the three bombs analysed by Philip, she found that a simple<br />

relationship between impulse (I), charge weight <strong>and</strong> radius took the form<br />

I=K 1 W 2/3 /R,<br />

(1.25)<br />

Figure 1.9 Relationship between scaled duration <strong>and</strong> scaled range (from Philip, ref.<br />

1.15).

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