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| DOE-HDBK-1184-2004
NOTE: In Table 5-8, A and Z for organic and rust are based on the sum of the
elements of the empirical formula. ∆ for organic and rust are an average
of a range of values from the Handbook of Chemistry and Physics (CRC,
1973). A and Z for hydrides are based on the metal only, since hydrogen
is a minor contribution. ∆ for hydrides are taken from Richardson, 1999
and Cheng, 1999a. Hydrogen in tritium-labeled compounds has been
represented as protium only, as this has a minor effect on the ratio A/(Z∆).
Functional representations (curve-fits) of numerically calculated SAF data (for
monodisperse physical particle sizes), as a function of particle size, were further
derived. These representations are a refinement of those by Kropf (1998), and
more accurately fit the data at small particle sizes.
From the functional representations of SAFs for monodisperse physical particle
sizes, SAFs for polydisperse AMAD particle size distributions were calculated using
the methodology adapted from Kropf (1998) and Cheng (1999a). The resulting
values are given in Tables 5-9 and 5-10.
Table 5-9. SAFe for Various ITP Materials and Polydisperse (s g = 2.5) Particle Size
Distributions (in AMAD)
A/( Z∆)
SAF e vs. Particle Size [AMAD(m), s g=2.5]
Base Material*
10
5
2
1
0.5
Organic [∼(CH2)n]
1.944
0.305 0.474
0.707
0.841
0.925
Rust [∼FeO(OH)]
0.690
0.231 0.381
0.614
0.768
0.879
Ti H2
0.558
0.215 0.362
0.594
0.753
0.871
Zr H2
0.351
0.180 0.312
0.541
0.714
0.852
Hf H2
0.212
0.142 0.260
0.490
0.680
0.842
* Variable amounts of elemental hydrogen are isotopically tritium.
Table 5-10. SAFβ for Various ITP Materials and Polydisperse (s g = 2.5)
Particle Size Distributions (in AMAD)
A/( Z∆)
SAFβ vs. Particle Size [AMAD(m), σ g=2.5]
Base Material*
10
5
2
1
0.5
Organic [∼(CH2)n]
1.944
0.205
0.333 0.535 0.677
0.789
Rust [∼FeO(OH)]
0.690
0.140
0.244 0.439 0.602
0.745
Ti H2
0.558
0.133
0.231 0.423 0.590
0.739
Zr H2
0.351
0.104
0.191 0.380 0.555
0.719
Hf H2
0.212
0.077
0.154 0.343 0.529
0.707
* Variable amounts of elemental hydrogen are isotopically tritium.
Other published computations of self-absorption factors (Richardson, 1999; Traub,
1999) largely confirm the results above. Traub (1999) states that bremsstrahlung
photons, created when beta particles are self-absorbed, are not expected to be a
significant contribution to dose from tritiated particulates.
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