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Nuclear Spectroscopy

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E X P E R I M E N T 13<br />

Uranium 238 Series<br />

INTRODUCTION<br />

Like thorium, uranium is found is most building<br />

materials and soils on the earth. There are three<br />

isotopes of uranium still found abundantly in the<br />

earth’s crust. Mass 238 is the most abundant (99.28%),<br />

and the other isotopes are much less abundant, 235 U<br />

(0.72%), 234 U (0.0055%).<br />

The vast difference in the relative abundances of 238 U<br />

and 235 U is supposedly due to the factor of 6 difference<br />

in their half-lives (see Tables 13.1 and 13.2), and<br />

the long time from the creation of nearly equal<br />

quantities of the two isotopes. This was about 6 x 10 9<br />

years ago, the postulated time for the supernova<br />

whose remnants eventually became our solar system.<br />

The presence of 234 U after this great length of time is<br />

due only to its being created in the decay chain<br />

(shown in Figure 13.1 and 13.2) starting with 238 U.<br />

235<br />

U has its own decay chain, ending with the stable<br />

isotope, 207 Pb. For most environmental measurements,<br />

gammas from isotopes in the 235 U decay series<br />

are too weak to observe with small NaI(Tl) detectors.<br />

Table 13.1<br />

U-238 4.47 x 10 9 yr 1.41 x 10 17 sec<br />

Th-234 24.1 day 2.08 x 10 6 sec<br />

Pa-234 1.17 min 68.4 sec<br />

U-234 2.46 x 10 5 yr 7.76 x 10 12 sec<br />

Th-230 7.54 x 10 4 yr 2.38 x 10 12 sec<br />

Ra-226 1.6 x 10 3 yr 5.05 x 10 10 sec<br />

Rn-222 3.8235 day 3.30 x 10 5 sec<br />

Po-218 3.10 min 186 sec<br />

Pb-214 26.8 min 1.61 x 10 3 sec<br />

Bi-214 19.9 min 1.19 x 10 3 sec<br />

**Po-214 163.7 µsec 1.64 x 10 -4 sec<br />

**Tl-210 1.3 min 78 sec<br />

Pb-210 22.3 yr 7.04 x 10 8 sec<br />

Bi-210 5.01 day 4.33 x 10 5 sec<br />

Po-210 138.38 day 1.20 x 10 7 sec<br />

Pb-206 stable<br />

226<br />

Ra<br />

88<br />

63.3 (3.8%)<br />

92.6 (5.4%)<br />

234 γ Th<br />

90<br />

1001.6 keV (0.6%)<br />

γ 67.7 keV (23.4%)<br />

230<br />

Th<br />

90<br />

234<br />

Pa<br />

91<br />

Figure 13.1 The uranium decay series to radium.<br />

238<br />

U<br />

92<br />

The 238 U decay chain contains radium ( 226 Ra) and<br />

radon ( 222 Rn) isotopes discovered by Marie and Pierre<br />

Curie at the beginning of the 20th century. This radon<br />

isotope is the one that seems to worry some health<br />

physicists and environmentalists the most, as far as its<br />

concentration in houses, mines, and buildings. You<br />

will handle sources with radon and radium in some lab<br />

exercises below. Your exposure to these isotopes will<br />

not be any more health-threatening to you than exposure<br />

to other isotopes suggested for use in this book of<br />

experiments. As always, proper handling of radioisotopes<br />

should always be followed, whether they pose a<br />

significant or insignificant health risk. Whether exposure<br />

to radon is a health risk or a benefit has been<br />

called into question (see Cohen).<br />

Radon will only appear as a significant isotope in<br />

naturally occurring uranium ores. Uranium compounds<br />

from the chemistry lab have not had enough<br />

time to populate 226 Ra significantly because of the long<br />

uranium half-lives. The resulting activity of 222 Rn is the<br />

same as 226 Ra, very small.<br />

γ<br />

U<br />

234<br />

92<br />

γ 53.2 keV (28%)<br />

40

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