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Untitled - Sciencemadness Dot Org

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0.350 I I I I I<br />

.c<br />

3 O-.-----<br />

l-0 0 o-0 -0<br />

0.250<br />

” 0.300<br />

SHOCK INITIATION PROPERTIES<br />

0 = PRECIPITATED<br />

0 = BALL-MILLED<br />

4-O<br />

Fig. 4.19. Small-scale gap test sensitivity of RDX vs<br />

specific surface at loading density = 0.80 g/cm3.<br />

0.350 I I I I I<br />

0.2ccJ<br />

0 = PRECIPITATED<br />

0 = BALL-MILLED<br />

I I I I I I<br />

2000 4OW 6OCG SO00 I0000 12ocm<br />

s,’ kn12/g 1<br />

Fig. 4.20. Small-scale gap test sensitivity of RDX vs<br />

specific surface at loading density = 1.00 g/cm3.<br />

4.3. Minilmum Priming Charge. The minimum priming charge test determines<br />

the quantity of some initiator or booster explosive that will cause high-order<br />

detonation in the test explosive in half the trials. This test has been used to deter-<br />

mine both the relative effectiveness of various initiator explosives and the relative<br />

sensitivities of various test explosives. The basic property of the test explosive is its<br />

ability to build up to a high-order detonation after a short, intense, geometrically<br />

small, and usually highly divergent shock wave is induced from the priming charge.<br />

Figure 4.21 shows the LASL version of this test. The test charge is a 2-in.-diam by<br />

2-in.-high cylinder. A hemispherical cavity milled into one face is filled with a<br />

putty-like explosive, XTX 8003, prepared by roll-milling 80 parts of a specially<br />

recrystallizied PETN with 20 parts of an uncatalyzed silicone resin (Dow Corning<br />

-1<br />

433

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