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| DOE-HDBK-3010-94
4.0 Solids; Summary
value as designated by the authors is chosen. The measured values were only
for airborne particles <10 m AED. The values for solubility class in
simulated lung fluids are assumed to be >95% "Y" class with remainder in
"D" class, based on the solubilities of sintered oxides recovered from the burn
tests performed as part of the hazard classification tests on armor-defeating
munitions.
The 95% confidence level airborne release value for oxidation of uranium
metal at flow velocities <100 cm/s reported by Carter and Stewart (September
1970) is exceeded by the value reported by Elder and Tinkle (December 1980)
during the oxidation of staballoy penetrators in laboratory experiments. The
ARF x RF values obtained for experiments at temperatures less than 900 oC
were less than 1E-3. ARF and RF values of 1E-3 and 1.0 are assessed to be
bounding for this category with the solubility classification for the oxides
formed given above.
Median
ARF 1E-4/RF 1.0
Bounding
ARF 1E-3/RF 1.0
Airborne release during free-fall of molten metal drops. The median
ARF x RF values for free-fall of molten uranium metal droplets in air are as
given by Carter and Stewart (1970). The ARF x RF value assessed to be
bounding is an arbitrary increase of the 95% confidence level value assigned
by Carter and Stewart (to 1E-2) to be consistent with the comparable value for
plutonium. Since the airborne material is cooled rapidly after formation, the
solubility of the airborne oxides formed from plastic deformation and ignition
of the thin film of metal generated by the impact of penetrators against hard
targets is assessed to be 50% "Y" class and 50% "D" class.
Median
ARF 2E-3/RF 1.0
Bounding
ARF 1E-2/RF 1.0
Airborne release from explosive dispersal of molten uranium. The values for
explosive release of molten uranium indicate that, if the uranium is molten and
subdivided in very small drops (as by the exploding wire technique) and
ejected into air at sonic velocities (as by the electrodynamic thruster technique
described), all the uranium could be made airborne as a very fine particulate
material with all particles or aggregates 10 m AED and less (Rader and
Benson, June 1988). The solubility class of the airborne material is
anticipated to be like the airborne material formed during impact of staballoy
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