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A History of Research and a Review of Recent Developments

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10<br />

The nature <strong>of</strong> explosions<br />

Figure 1.1 Overpressure/duration curve for detonation in air (idealization with<br />

exponential decay) (from Friedl<strong>and</strong>er, ref. 1.19).<br />

<strong>of</strong> TNT generates a blast energy <strong>of</strong> approximately 4600 joules/gram, which is<br />

equivalent to about 1100 calories/gram. In fact, the definition <strong>of</strong> a ‘st<strong>and</strong>ard’<br />

gram <strong>of</strong> TNT is that which gives a blast energy <strong>of</strong> 4610 joules. The definition<br />

<strong>of</strong> a st<strong>and</strong>ard ton <strong>of</strong> TNT is an energy release <strong>of</strong> one million kilo-calories.<br />

For a given type <strong>of</strong> chemical high explosive, energy is proportional to total<br />

weight, so it has become customary for design purposes to rewrite Eq. (1.1) as<br />

p =K W/R (1.2)<br />

0 1<br />

K1 is no longer non-dimensional <strong>and</strong> great care must be used in applying the<br />

formula. Experiments suggested that the equation did not give very accurate<br />

values <strong>of</strong> p0 over the entire range, <strong>and</strong> an improved version was proposed in<br />

the US Army Technical Manual Fundamentals <strong>of</strong> Protective Design (Non-nuclear),<br />

No. TM5–855–1, published originally in 1965 [1.10]. In imperial units the<br />

equation became<br />

3 .<br />

(1.3)<br />

where<br />

p0=peak pressure in psi<br />

z=R/W 1/3<br />

(R in feet, W in lb).<br />

The relationship should only be applied when 160>p0>2 psi, <strong>and</strong><br />

20>R/W 1/3 >3 ft/lb 1/3 .

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