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DETONATION PROPERTIES<br />

Table 3.48 DETONATION FAILURE THICKNESS<br />

Failure<br />

Density Thickness<br />

Explosive k/cm? (mm)<br />

Pure Explosives<br />

Ammonium picrate 1.64 3.29<br />

TNT 1.61 1.91”<br />

Castable Mixtures<br />

Comp A-3 1.63 0.57<br />

Comp B-3 1.72 0.94<br />

Cyclotol75/25 1.75 1.51<br />

Octal 75/25 1.79 1.43<br />

Pentolite 1.70 1.39b<br />

HMX-Based<br />

PBX 9011<br />

PBX 9404<br />

X-0204<br />

RDX-Based<br />

PBX 9010<br />

PBX 9205<br />

PBX 9407<br />

“Pressed at 65°C.<br />

Tast SO-mm wedge.<br />

Plastic-Bonded Explosives<br />

1.77 0.61<br />

1.83 0.46<br />

1.922 0.41<br />

1.78 0.52<br />

1.69 0.57<br />

1.77 0.30<br />

A linear curve is fitted through the data and extrapolated to 0”, and the failure<br />

thickness at 0” is designated the detonation failure thickness.<br />

If the brass plate were completely incompressible, the failure thickness so deter-<br />

mined would be half that of an unconfined infinite sheet. The failure thickness of an<br />

unconfined sheet is less than the failure diameter of a cylinder because rarefactions<br />

in a cylinder enter from all sides of the charge and influence the detonation. Thus,<br />

the failure diameter may be several times the failure thickness and may vary from<br />

one explosive to another.<br />

More complete details are given in a LASL report.s<br />

REFERENCES<br />

1. W. E. Deal, Journal of Chemical Physics 27(l), 796-800 (September 1957).<br />

-2. Louis C. Smith, Explosivstoffe 15, 106-110, 130-134 (1967).<br />

3. Manuel J. Urizar, Suzanne W. Peterson, and Louis C. Smith, Los Alamos<br />

Scientific Laboratory report LA-7193-MS (April 1978).<br />

290

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