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DOE-HDBK-3010-94
4.0 Solids; Metals
munitions prior to deployment (Gilchrist, Parker and Mishima, March 1978; Hooker et
al., March 1985; Haggard et al., July 1986; Parkhurst et al., March 1990). A pre-
determined number of boxes of munitions are subjected to an intense wood-fuel oil
fire. The distance large fragments (pieces of munitions components and cases,
packing) are ejected and the thermal and blast levels are determined to establish the
exclusion area requirements in the event of accidents in transport and storage. In all
cases, no airborne DU was collected in the air samplers set downwind at various
distances downwind of the fire. Size distributions of the residual oxide powders
(predominantly U3O8) were determined and estimates of the respirable fraction are
based on the presence of particles of 10 m and less AED in the residual oxide. The
size distributions measured show less than 0.01 of the residual oxides are in the
respirable size range. The material in the respirable fraction is much less soluble than
the airborne oxide from impact tests ranging from 96% to 100% in the "Y" class.
From the data reproduced in Figure 4-11 from Carter and Stewart (1970), a geometric
mean ARF x RF of 1E-4 was reported. The 95% confidence level ARF x RF of
4E-4 reported by Carter and Stewart (1970) is exceeded by the ARF and RF estimated
for tests performed by Elder and Tinkle (December 1980), where the gas flow and
temperatures used exceeded those used by Carter and Stewart (1970). Six of nine
ARF x RF values obtained are less than 1E-3, with the greater values at the higher
temperatures (900 oC). The ARF and RF values of 1E-3 and 1.0 are assessed to be
bounding for this thermal stress configuration. The value for the lung solubility class
is assumed to be that determined for the sintered oxides collected from wood-oil fires
involving DU rods in munitions (i.e., >95% "Y" class with the remainder being "D"
class uranium). This value is assessed to be bounding for the issue of lung solubility
class.
4.2.1.2.2 D istu rb ed M olten M etal S u rface W ith H igh T u rb u len ce. Carter and
Stewart performed a series of experiments to measure the characteristics of airborne uranium
from molten metal under static (no metal movement) and dynamic (free-fall drop) conditions.
The experimental apparatus and procedures were covered in subsection 4.2.1.1.4. The size
distributions of the airborne materials are shown in Figure 4-11 reproduced from that
document (the velocity of the updraft through the vertical tube was set at a velocity to carry
particles <30 m AED). The distribution of airborne material from the experiments under
static conditions appears to be a single mode. The airborne material from experiments under
dynamic conditions (2 to 4 m free-fall) are bimodal. The distribution from the experiments
in which "obvious sparking" was observed appears to fit the coarser (upper) curve with the
finer (lower) curve represented by the airborne material under static conditions.
Page 4-42


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