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Introduction to Health Physics: Fourth Edition - Ruang Baca FMIPA UB

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112 CHAPTER 4<br />

TABLE 4-1. Thorium Series (4n)<br />

ENERGY (MeV)<br />

GAMMA (PHOTONS/<br />

NUCLIDE HALF-LIFE ALPHA a BETA TRANS.) b<br />

232<br />

90Th 1.39 1010 yrs 3.98<br />

228<br />

88Ra (MsTh1) 6.7 yrs 0.01<br />

228<br />

89Ac (MsTh2) 6.13 h Complex decay scheme 1.59 (n.v.) 0.966 (0.2)<br />

Most intense beta<br />

group is 1.11 MeV<br />

0.908 (0.25)<br />

228<br />

90Th (RdTh) 1.91 yrs 5.421 0.084 (0.016)<br />

224<br />

88Ra (ThX) 3.64 d 5.681 0.241 (0.038)<br />

220<br />

86Rn (Tn) 52 s 6.278 0.542 (0.0002)<br />

216<br />

82Po (ThA) 0.158 s 6.774<br />

212<br />

82Pb (ThB) 10.64 h 0.35, 0.59 0.239 (0.40)<br />

212<br />

83Bi (ThC) 60.5 min 6.086 (33.7%)c 2.25 (66.3%) c 0.04 (0.034 branch)<br />

212<br />

84Po (ThC′ ) 3.04 × 10−7 s 8.776<br />

208<br />

81Tl (ThC′′ ) 3.1 min 1.80, 1.29, 1.52 2.615 (0.997)<br />

208<br />

82Pb (ThD) Stable<br />

aOnly the highest-energy alpha is given. Complete information on alpha energies may be obtained from Sullivan’s Trilinear Chart of<br />

Nuclides, Government Printing Office, Washing<strong>to</strong>n, DC, 1957.<br />

bOnly the most prominent gamma rays are listed. For the complete gamma-ray information, consult T. P. Kohman: Natural<br />

radioactivity, in H. Blatz (ed.): Radiation Hygiene Handbook. McGraw-Hill, New York, 1959, pp. 6–13.<br />

cIndicates branching. The percentage enclosed in the parentheses gives the proportional decay by the indicated mode.<br />

All of the iso<strong>to</strong>pes that are members of a radioactive series are found in the upper<br />

portion of the periodic table; the lowest a<strong>to</strong>mic number in these groups is 81, while<br />

the lowest mass number is 207.<br />

All the radioactive series have several common characteristics. The first member of<br />

each series is very long-lived, with a half-life that may be measured in geological time<br />

units. That the first member of each must be very long-lived is obvious because, if the<br />

time since the creation of the world is considered, relatively short-lived radioactive<br />

material would have decayed away during the 4.5 billion years that the earth is<br />

believed <strong>to</strong> have been in existence. This point is well illustrated by considering the<br />

artificially produced neptunium series. In this case, the first member is the transuranic<br />

element 241 Pu, which is produced in the labora<strong>to</strong>ry by neutron irradiation of reac<strong>to</strong>rproduced<br />

239 Pu. The half-life of 241 Pu, however, is only 13 years. Because of this short<br />

half-life, even a period of a century is long enough <strong>to</strong> permit most of the 241 Pu <strong>to</strong><br />

decay away. Even the half-life of the longest-lived member of this series, 237 Np, which<br />

is 2.2 × 10 6 years, is sufficiently short for this element <strong>to</strong> have essentially disappeared<br />

if it had been created at the same time as all the other elements of the earth.<br />

A second characteristic common <strong>to</strong> all three naturally occurring series is that each<br />

has a gaseous member and, furthermore, that the radioactive gas in each case is a<br />

different iso<strong>to</strong>pe of the element radon. In the case of the uranium series, the gas<br />

(Rn) is called radon; in the thorium series, the gas is called thoron; and in the actinium<br />

series (Table 4-4), it is called actinon. It should be noted that the artificial neptunium<br />

series (Table 4-2) has no gaseous member. The existence of the radioactive gases in

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