Occupational Intakes of Radionuclides Part 1 - ICRP
Occupational Intakes of Radionuclides Part 1 - ICRP
Occupational Intakes of Radionuclides Part 1 - ICRP
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DRAFT REPORT FOR CONSULTATION<br />
2376 Table 6 Central values <strong>of</strong> dissolution parameters for Type F, M, and S material from a review<br />
<strong>of</strong> experimental data a<br />
2377<br />
Type F(fast) M (moderate) S (slow)<br />
Fraction dissolved rapidly<br />
Dissolution rates:<br />
fr 0.95 (0.84) [1.4] 0.20 (0.18) [4] 0.007 (0.003) [9]<br />
Rapid (d-1) sr 12 (9) [8] 1.7 (1.5) [9] 2.0 (3.8) [14]<br />
Slow (d-1) ss 0.02 (0.02) [8] 0.003 (0.003) [4] 0.00018 (0.00008) [9]<br />
2378<br />
2379<br />
a<br />
Median value, with geometric mean in parentheses, and geometric standard deviation in<br />
2380<br />
2381<br />
brackets.<br />
2382 (149) Updated default values, given in Table 7, were based mainly on the following<br />
2383 considerations, but also take account <strong>of</strong> the large uncertainties in the central values<br />
2384<br />
2385<br />
and the need for simple rounded numbers.<br />
2386 Rapid fraction fr:<br />
2387 (150) For Type F, the median value (0.95) is close to the current default value <strong>of</strong><br />
2388 1.0. For simplicity in implementation it is preferable not to change to two-phase<br />
2389 dissolution. The default value remains 1.0.<br />
2390 For Type M, the median value is higher (0.20) than the current default (0.1). The<br />
2391 updated default value is taken to be 0.2.<br />
2392 For Type S, the median value is higher (0.007) than the current default (0.001).<br />
2393<br />
2394<br />
The updated default value is rounded to 0.01.<br />
2395 Rapid dissolution rate, sr:<br />
2396 (151) Type F: the median <strong>of</strong> values <strong>of</strong> sr estimated from experimental data for<br />
materials that would be assigned to Type F, is 12 d –1 2397<br />
(Table 5), (much lower than the<br />
original HRTM default value <strong>of</strong> 100 d –1 2398<br />
). However, this outcome is heavily<br />
2399 influenced by results for a few elements: about half <strong>of</strong> the results are from only four<br />
2400 elements. To include information from a wider range <strong>of</strong> elements in choosing the<br />
2401 default value, consideration was also given to the element-specific values <strong>of</strong> sr for<br />
2402 soluble (Type F) forms <strong>of</strong> the element, which were assessed where suitable<br />
2403 experimental information was available (see above). There are element-specific<br />
2404 values for several elements for which no material-specific values were assessed.<br />
2405 Hence the distribution <strong>of</strong> element-specific values covers a wider range <strong>of</strong> elements,<br />
2406 and in it each element makes the same contribution (one entry): its median value is 50<br />
d –1 2407 . Taking both medians into account, the updated default value <strong>of</strong> sr for Type F is<br />
taken to be 30 d –1 2408<br />
.<br />
2409 (152) Types M and Type S: The medians <strong>of</strong> estimated values <strong>of</strong> sr for materials that<br />
would be assigned to Types M and S, are 1.7 d –1 , and 2 d –1 2410<br />
, respectively (Table 5),<br />
(very much lower than the original HRTM default <strong>of</strong> 100 d –1 2411<br />
). As for Type F, the<br />
2412 distributions are heavily influenced by results for a few elements. For Type F,<br />
2413 consideration <strong>of</strong> element-specific values <strong>of</strong> sr involved a wider range <strong>of</strong> elements, and<br />
2414 led to the choice <strong>of</strong> a somewhat higher value than the material-specific values.<br />
2415 However, whereas for Type F materials the rapid dissolution rate, sr, represents<br />
2416 overall absorption, and is assumed to be element-specific, for Type M and S materials<br />
2417<br />
sr is more likely to be determined by dissolution <strong>of</strong> the particle matrix, and so less<br />
68