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DOE-HDBK-3010-94
4.0 Solids; Summary
P ow d ers
For low-energy stresses, powders do not tend to significantly fragment. For high-energy
stresses considered in this document, the size fraction of powders of concern have relaxation
times on the order of fractions of a millisecond, and thus do not tend to present themselves
for fragmentation. Therefore, the amount of respirable material assumed airborne using this
handbook should not exceed the amount of respirable material originally present in the source
MAR, if that value is known. If the value is not known, and the bounding value specifically
uses as the RF the fraction of original MAR less than 10 m AED, an RF of 0.1 can be
assumed based on Ayer, et al. ( May 1988).
T h erm al S tres s
The ARFs and RFs assessed to be bounding for various plutonium compounds subjected to
thermal stress (temperature <1000 oC, natural convection) are given below. For the
chemically non-reactive compounds in powder form, suspension is from the entrainment of
pre-formed particles by the flow upwards from the heated surface. The mass of particles in
any size range (respirable size) released cannot exceed the total mass of particles in the
source powder since no new particles are formed. For the reactive compounds in powder
form, the release is dependent on the particles formed by the reaction (oxidation in the
experiments presented) and the phenomena that would carry the particles formed into the
local flow field. Thus, some variation is anticipated.
Bounding
(non-reactive compounds)
ARF 6E-3/RF 1E-2
(reactive compounds except PuF4)
ARF 1E-2/RF 1E-3
(PuF4)
ARF 1E-3/RF 1E-3
E xp losive S tres s
The effect most closely resembling stresses in a given explosive-type accident scenario is
chosen. There is no need to assume cumulative releases for all effects cited.
Shock effects. Based upon data for cratering and associated airborne release
of soil a respirable release of the mass of inert material equal to 20% of the
calculated TNT equivalent is assessed to be bounding for detonations in or
contiguous to powder in open air where shock and blast effects will quickly
disperse. The mass of the material-of-concern is dependent upon the
concentration of the material-of-concern in the powder.
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