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4.0 Solids; Powders
Table 4-11. ARFs and RFs During the Heating of Reactive Compounds in Flowing Air
(Tables VI, VIII & X - Mishima, Schwendiman and Radasch, July 1968
and Table IV - Mishima, Schwendiman and Radasch, November 1968)
Temperature, oC
ARF1
Air Velocity, cm/s
Air-Dried Plutonium Nitrate
10
1000
6.2E-5
50
400
1.9E-5
700
2.3E-4
1.5E-32
1000
100
400
1.7E-4
700
1.3E-4
1000
1.9E-4
1.3E-4
1
Sum of material collected on foil chimney liner and filter sealing chimney.
2
Size distributions determined by optical microscopy indicates a RF <1E-5 to <1E-8. May
indicate that oxides formed at high temperatures sinter together during oxidation forming
aggregates that are larger in size.
The maximum and median ARFs for fluoride appear to be an order of magnitude less with
less variability for individual measurements. Therefore, a bounding ARF value is assessed
to be 1E-3 for this compound.
The upsweep air velocities used during the tests appears to be adequate to entrain all
significant particle sizes as shown in Figure 4-14 reproduced from Mishima, Schwendiman
and Radasch (November 1968). The size distributions of the airborne materials during the
heating of some compounds are shown in Figures A.28, A.29a, A.29b, A.29c and A.30 in
Appendix A. The sizes designated on the graphs are equivalent spheres (the linear diameter
of the particle) and, since the theoretical density of PuO2 is 11.46 g/cm3, the sizes must be
multiplied by 3.4 (the square root of the density) to arrive at the approximate diameters in
AED. The RF estimated from the size distribution plots indicate a value ~ 1E-5 to 1E-8
associated with ARFs ranging from <7E-4 to 8E-3. Although the RFs measured appear
relatively consistent associated with ARFs spanning the range of ARFs found for all
materials, the values are very small and a RF of 1E-3 is assessed to be bounding for all these
materials under these conditions to provide a high degree of conservatism.
Page 4-59
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