FRACTION, F, OF NUCLEI! ABLE TO ESCAPE (%)

108

100

R

d= diameter
R= recoil range

he: d/R

d = thickness
fe d/R
R = recoil range

2

4

6

8

10

i2

14

IS

p= (PARTICLE SIZE/RECOIL RANGE)

Fic. 85.—-Theoretical escape of recoiling atoms from spherical and planar particles
TABLE 48.

Tissue

Author

Liver

Reference

| Duration, years|

™8Ra/2Th

28Th/28Ra

24Ra /28Th

22Ph /24Ra

tundo

2

13.5-14.5

Hursh
Baserga

34
35

20
15

0.62 (2)
[0.62-0.625]

0.76 (2)
[0.73-0.80]

0.66 (2)
[0.66-0.67]

0.42 (2)
[0.39-0. 45]

0.46 (1)

0.90 (3)
(0. 87-0. 92]

—

—

Kaul

! Parr et al.

|
Spleen

{undo

Hursh

Kaul

Parr et al.
Trabecular

bone

Marinelli et

without marrow |

al.

, Kaul

Parr et al.
Red bone marrow

Sreapy-State Activrry Ratios 1n Man (BURDENS 1 YEAR)

Kaul
an et al.

6, 7
| This paper

long term (?)

—
0.41 (1)

11-26

0.36 (1)

13.5-14.5

0.69 (1)

6,7

long term (?)

This paper

11-26

0.72 (3)
[(0.33-1.07]
0.36 (1)

2

34

11
6, 7

| This paper
6, 7
This paper

20

15-26.5
long term (?)

26
long term (?)
- 11-26

0.48 (1)

1.6 (1)
1.3 (3)
[1.2-1.5]

—

0.23 (3)
f0.19-G.30]
_

0.9 (1)
0.88 (1)

—
—

—_—
—

1.00 (2)

0.75 (1)

—-

0.83 (1)

0.75 (1)

0.17 (1)

0.91 (4)
[0.85-0.96]
1.00 (2)
{0.97-1.03]

0.90 (3)
(0.89-0.91}
0.74 (1)

1.09 (7)

—

—

1.2 (7)
{1.1-1.7]

1.0 (1)

—

1.0 (1)

7 (1)

—

1.12 (3)
[1.08-1.18]
1.05 (2)
1.0-1.1

—

—

0.59 (2)
[0. 58-0. 60]

—

[1.00-1.01] -

0.96 (1)

(0. 64-1. 48]

—

|?!

—

0.57 (3) |
[0.44-0.84] |
—

() Figures in — parentheses quote the number of measurements. Figures in square parentheses quote the range.

viously places this nuclide on a very sensitive part of

the curve. Perhaps this accounts for some of the vari-

ability in results obtained with different batches of
Thorotrast. It is also significant that at late times after
Thorotrast administration, the particles are present in
the form of aggregates, and the escape of **8Ra appears
to be further impeded. Thus, steady state activity ratios, ““8Ra/**?Th, of the order of 0.5 are then reported

(see Table 48). Presumably this higher retenti

be explained by the recoil of 7 8Ra atoms from o:
ticle into another in such a way that they cont:
be trapped.
The interpretation of the estimated 2?°TI

steady state activity ratios, fe, presents consi:
difficulties (see appendix). From the results of

term experiments, the calculated values of (1 —
peal

fy)

roet

1

rr

Select target paragraph3