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R. Meyer J. Köhler A. Homburg Explosives

R. Meyer J. Köhler A. Homburg Explosives

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Detonation<br />

which the safety distance (in meters) is calculated from the expression<br />

f· 3<br />

öäM where M is the maximum amount of explosives in kg which are<br />

present in the building at any time, whereas f is a factor which varies,<br />

according to the required degree of safety, from 1.5 (distance between<br />

two barricaded store houses) to 8 (distance from the non-dangerous<br />

part of the plant). The f-value stipulated by the regulations may be as<br />

high as 20 for residental areas in the vicinity of the plant.<br />

The shock wave theory is easier to understand, if we consider a planar<br />

shock wave, such as the one shown in Fig. 11, on the assumption that<br />

the tube is indestructible (such shock wave tubes are utilized as<br />

research instruments in gas dynamics and in solid state physics; the<br />

shock sources are explosions or membranes bursting under pressure).<br />

Comparative treatment of the behavior of the gas in the tube yields the<br />

following relationships.<br />

From the law of conservation of mass:<br />

r0D = r1(D–W) or v1D = v0(D–W) (1)<br />

From the law of conservation of momentum:<br />

p1 – p0 = r0DW or v0(p1 – p0) = DW (2)<br />

From the law of conservation of energy:<br />

p1W = †0D (e1 – e2 + W2<br />

); (3)<br />

2<br />

Rearrangements yield the so-called Hugoniot equation:<br />

e1 – e0 = 1<br />

2 (p1 + p0) (v0 – v1) (4)<br />

Equation (4) represents a curve in the p – vdiagram, the Hugoniot<br />

curve.<br />

The following expression is obtained for the velocity D of the shock<br />

wave and for the velocity of matter W:<br />

p1 – p0<br />

D = v0 öäää v0 – v1<br />

and<br />

W = öääääääääääää<br />

(p1 – p0) (v0 – v1) (6)<br />

These relationships are valid irrespective of the state of aggregation.<br />

2. Detonation Wave Theory<br />

If the medium is explosive, an explosive chemical reaction must be<br />

produced immediately in the wave front because of the drastic tem-<br />

80<br />

(5)

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