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Page Title: Table 4-5. Measured ARFs During the Self-Sustained Air Oxidation of Large Specimens of Unalloyed and Delta Plutonium Metal
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DOE-HDBK-3010-94
4.0 Solids; Metals
variations for the measurements would be a factor of ~ 20. The fraction of the residual
powder 20 m AED and less was <3.1E-4. The material was friable and the value may
represent some fraction of material fragmented during sieving.
Mishima (November 1966) reported the ARFs and RFs from the self-sustained air oxidation
of four large specimens of delta-phase and unalloyed plutonium metal. The three unalloyed
pieces ranged in mass from 455.5 g to 1770 g. The single delta-stabilized specimen was
997 g. The metal specimen was placed within a ring made of insulating material set upon a
sheet of insulating material (the metal would not sustain ignition in the absence of the
insulating material due to heat transfer to the metal enclosure). The top surface of the metal
specimen was ignited with a heliarc torch. Air was drawn into a quartz chimney placed
within one inch of the metal surface at a nominal velocity of 525 cm/s through the 2.685-in.
(68-mm) i.d. chimney. Airborne material was collected on a glass fiber filter sealing the end
of the chimney. Air was drawn through a side arm at 550 to 800 cm/s to collect airborne
materials on a membrane filter for size distribution analysis by transmission electron
microscopy. The experimental apparatus is shown in Figure A.16 and the results reproduced
in Table A.25 in Appendix A. The size distribution measured for material airborne during
oxidation of the largest metal specimen, considered representative of all measurements, is
reproduced as Figure A.17 in Appendix A. Pertinent data are listed in Table 4-5.
Table 4-5. Measured ARFs During the Self-Sustained Air Oxidation
of Large Specimens of Unalloyed and Delta Plutonium Metal
(Table II - Mishima November 1966)
Total Sampling
Weight Metal (g)
Time (min)
Form
ARF
90
569.8
Unalloyed
4.9E-4
45
1770
Unalloyed
1.4E-4
22
997
Delta
3.4E-5
60
455.5
Unalloyed
3.9E-6
With the limited data base, the ARFs do not appear to correlate with any measured
parameter (mass, form) but Haschke (July 1992) reports that the airborne release is time-
dependent. The largest ARF, ~ 5E-4, is in the range of but exceeds the 95% confidence
level value (1E-4) specified by Carter and Stewart (1970). Although the masses are larger,
the duration required for complete oxidation to self-extinguishment appear to be much less
than required for much smaller specimens used by Mishima (December 1965) and the ARFs
are two to four orders of magnitude larger. The principal differences between the conditions
under which these measurements and the previous measurements were made are the specimen
masses (larger) and air flow patterns (up and around at higher nominal velocities).
Page 4-24


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