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R. Meyer J. Köhler A. Homburg Explosives

R. Meyer J. Köhler A. Homburg Explosives

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25 Ballistic Bomb<br />

z(p/pmax) = p/pmax/{1 + x(1 – p/pmax)} (4)<br />

and<br />

p(z) = F * z / (1 + xz). (5)<br />

Accordingly, the maximum gas pressure achieved at the end of burnup<br />

(z = 1) is calculated as<br />

pmax = F / (1 + x). (6)<br />

The dynamic liveliness L is calculated from<br />

L = S(0) ˙e(pref)<br />

* f(z) * *<br />

V(0) pref [ p<br />

pref] a–1 1 + x<br />

*<br />

(1 + xz) 2<br />

S(0)/V(0) is the ratio of the initial surface area to the initial volume of<br />

the powder,<br />

f(z) is the shape function of the powder, which takes account of<br />

the geometrical conditions (sphere, flake, cylinder, N-hole<br />

powder) during the burn-up (f(z) = current surface area /<br />

initial surface area)<br />

˙e(pref) is the linear burning rate at the reference gas pressure pref<br />

pref<br />

is the reference gas pressure and<br />

a is the pressure exponent, which for many powders is close<br />

to 1.<br />

To evaluate Eq. (7), z should be replaced by p/pmax using Eq. (4).<br />

Figure 3 shows the time profile of the pressure in the manometric<br />

bomb for a typical 7-hole powder. Initially the pressure is increasingly<br />

steep, since burn-up takes place more quickly the higher the pressure<br />

and in addition the burning surface of the powder becomes greater as<br />

Fig. 3. Pressure-time graph p = f(t)<br />

(7)

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