The radioactive isotope ^{40}K (odd Z and odd N ) is naturally present in biological tissues and subjects humans to a certain amount of unavoidable internal radiation. The body of an adult weighing 70 kg contains about 170 g of potassium, mostly in intracellular fluids. The relative natural abundance of ^{40}K is 0.0118%, its half-life is 1.28\times 10^{9} years, and it emits b particles with an average kinetic energy of 1.40 MeV.
1. Calculate the total activity of ^{40}K, in millicurie, for a 70 kg adult.
2. Find the radiation dose rate in mrem/y.
Note: Potassium-40 is not included in Table 9.6 because human exposure to it is governed entirely by the body’s metabolic processes and its natural abundance. Therefore, it cannot be controlled by regulation.
TABLE 9.6 | |||||||
Calculated Concentrations (pCi/L) of \beta and Photon Emitters in Drinking Water Yielding a Dose of 4 mrem/year to the Total Body or to Any Critical Organ as Defined in NBS Handbook 69 | |||||||
Nuclide | pCi/L | Nuclide | pCi/L | Nuclide | pCi/L | Nuclide | pCi/L |
H-3 | 20,000 | Sr-85 m | 21,000 | Sb-124 | 60 | Er-169 | 300 |
Be-7 | 6,000 | Sr-85 | 900 | Sb-125 | 300 | Er-171 | 300 |
C-14 | 2,000 | Sr-89 | 20 | Te-125m | 600 | Tm-170 | 100 |
F-18 | 2,000 | Sr-90 | 8 | Te-127 | 900 | Tm-171 | 1,000 |
Na-22 | 400 | Sr-91 | 200 | Te-127m | 200 | Yb-175 | 300 |
Na-24 | 60 | Sr-92 | 200 | Te-129 | 2,000 | Lu-177 | 300 |
Si-31 | 3,000 | Y-90 | 60 | Te-129m | 90 | Hf-181 | 200 |
P-32 | 30 | Y-91 | 90 | Te-131m | 200 | Ta-182 | 100 |
S-35 inorg | 500 | Y-91 m | 9,000 | Te-132 | 90 | W-181 | 1,000 |
Cl-36 | 700 | Y-92 | 200 | I-126 | 3 | W-185 | 300 |
Cl-38 | 1,000 | Y-93 | 90 | I-129 | 1 | W-187 | 200 |
K-42 | 900 | Zr-93 | 2,000 | I-131 | 3 | Re-186 | 300 |
Ca-45 | 10 | Zr-95 | 200 | I-132 | 90 | Re-187 | 9,000 |
Ca-47 | 80 | Zr-97 | 60 | I-133 | 10 | Os-188 | 200 |
Sc-46 | 100 | Nb-93m | 1,000 | I-134 | 100 | Os-185 | 200 |
Sc-47 | 300 | Nb-95 | 300 | I-135 | 30 | Os-191 | 600 |
Sc-48 | 80 | Nb-99 | 3,000 | Cs-131 | 20,000 | Os-191m | 9,000 |
V-48 | 90 | Mo-99 | 600 | Cs-134 | 80 | Os-193 | 200 |
Cr-51 | 6,000 | Tc-96 | 300 | Cs-134m | 20,000 | Ir-190 | 600 |
Mn-52 | 90 | Tc-96m | 30,000 | Cs-135 | 900 | Ir-192 | 100 |
Mn-54 | 300 | Tc-97 | 6,000 | Cs-136 | 800 | Ir-194 | 90 |
Mn-56 | 300 | Tc-97m | 1,000 | Cs-137 | 200 | Pt-191 | 300 |
Fe-55 | 2,000 | Tc-99 | 900 | Ba-131 | 600 | Pt-193 | 3,000 |
Fe-59 | 200 | Tc-99m | 20,000 | Ba-140 | 90 | Pt-193m | 3,000 |
Co-57 | 1,000 | Ru-97 | 1,000 | La-140 | 60 | Pt-197 | 300 |
Co-58 | 300 | Ru-103 | 200 | Ce-141 | 300 | Pt-197m | 3,000 |
Co-58m | 9,000 | Ru-105 | 200 | Ce-143 | 100 | Au-196 | 600 |
Co-60 | 100 | Ru-106 | 30 | Ce-144 | 30 | Au-198 | 100 |
Ni-59 | 300 | Rh-103m | 30,000 | Pr-142 | 90 | Au-199 | 600 |
Ni-63 | 50 | Rh-105 | 300 | Pr-143 | 100 | Hg-197 | 900 |
Ni-65 | 300 | Pd-103 | 900 | Nd-147 | 200 | Hg-197m | 600 |
Cu-64 | 900 | Pd-109 | 300 | Nd-149 | 900 | Hg-203 | 60 |
Zn-65 | 300 | Ag-105 | 300 | Pm-147 | 600 | Tl-200 | 1,000 |
Zn-69 | 6,000 | Ag-110m | 90 | Pm-149 | 100 | Tl-201 | 900 |
Zn-69m | 200 | Ag-111 | 100 | Sm-151 | 1,000 | Tl-202 | 300 |
Ga-72 | 100 | Cd-109 | 600 | Sm-153 | 200 | Tl-204 | 300 |
Ga-71 | 6,000 | Cd-115 | 90 | Eu-152 | 200 | Pb-203 | 1,000 |
As-73 | 1,000 | Cd-115m | 90 | Eu-154 | 60 | Bi-206 | 100 |
As-74 | 100 | In-113m | 3,000 | Eu-155 | 600 | Bi-207 | 200 |
As-76 | 60 | In-114m | 60 | Gd-153 | 600 | Pa-230 | 600 |
As-77 | 200 | In-115 | 300 | Gd-159 | 200 | Pa-233 | 300 |
Se-75 | 900 | In-115m | 1,000 | Tb-160 | 100 | Np-239 | 300 |
Br-82 | 100 | Sn-113 | 300 | Dy-165 | 1,000 | Pu-241 | 300 |
Rb-86 | 600 | Sn-125 | 60 | Dy-166 | 100 | Bk-249 | 2,000 |
Rb-87 | 300 | Sn-122 | 90 | Ho-166 | 90 | ||
Source: From EPA, Implementation Guidance for Radionuclides, United States Environmental Protection Agency, Office of Ground Water and Drinking Water (4606M), EPA 816-F-00-002, March 2002, www.epa.gov/safewater. |
1. First calculate the decay rate constant, k, with units of s^{-1}
k=\frac{0.693}{t_{1/2}} =\frac{0.693}{(1.28\times 10^{9} y)(3.16\times 10^{7} s y^{-1})} =1.71\times 10^{-17} s^{-1}Let the number of {^40}K atoms = N
\mathscr{N} = \frac{170 g of K}{40.0 g/mol}\times (\frac{1.18\times 10^{-4} mol ^{40}K} {mol K})\times 6.02\times 10^{23} atoms/mol = 3.02\times 10^{20} atoms of ^{40}KActivity = \mathscr{A} = k\mathscr{N} = (1.71\times 10^{-17} s^{-1})(3.02\times 10^{20} atoms) = 5.16\times 10^{3} atoms/s(dps)
Converting to curies gives
2. Number of curies per kilogram = \frac{1.4\times 10^{-7} Ci} {70 kg} = 2.0\times 10^{-9} Ci/kg
Disintegrations per second per kilogram = \frac{5.16\times 10^{3} dps}{70 kg} = 73.7 s^{-1} kg^{-1}
Joules per \beta particle = (1.40\times 10^{6} eV)(1.60\times 10^{-19} J/eV) = 2.24\times 10^{-13} J
Joules × dps per kilogram = (2.24\times 10^{-13} J)(73.7 s^{-1} kg^{-1}) = 1.65\times 10^{-11} J/s/kg
Joules per kilogram per year = (1.65\times 10^{-11} J/s/kg)(3.16\times 10^{7} s/year) \\ = 5.22\times 10^{-4} J/kg=/year
The number of rems is the number of centijoules (10^{-2} J) of radiation energy absorbed per kilogram of tissue weight multiplied by the RBE factor. From Table 9.5, RBE = 1.
Since ^{40}K is distributed throughout all body tissues, we can assume that essentially all the \beta radiation energy is absorbed within the body.
Number of rem per year = \frac{5.22\times 10^{-4} J/kg/year} {10^{-2} J/kg/rem}
= 5.22\times 10^{-2} rem/year = 52.2 mrem/yearTable 9.7 shows that the annual dosage from all natural radiation sources received by a person is about 399 mrem, which shows that about 13% of our natural radiation exposure is from ^{40}K and is unavoidable because it is part of our body’s chemical makeup.
As shown in Table 9.7, about 84% of the total average annual effective dose is from natural sources of radiation, and of that, most is from radon. Of the other 16%, the majority is from medical diagnosis and treatments.
TABLE 9.5 | ||||
RBE (Relative Biological Effectiveness) Values for Several Types of Radiations, Based on Whole-Body Exposure | ||||
Radiation | RBE | |||
x- and \gamma-Rays | 1 | |||
\beta-Rays and electrons | 1 | |||
Thermal neutrons | 2 | |||
Fast neutrons | 10 | |||
High-energy protons | 10 | |||
\alpha Particles | 20 | |||
Fission fragments, heavy particles of unknown charge | 20 | |||
Heavy ions | 20 | |||
Note: RBE values are also called quality factors or weighting factors. |
TABLE 9.7 | ||||||
Sources of Environmental Radiation in the United States and Estimated Annual Dose Contributions to Individuals. The Total Annual Dose Is about 399 mrem/year | ||||||
Sources | Approximate Average Annual Dose to a Person in the United States (mrem/year) |
Approximate Percent of Total Dose Received |
||||
Natural sources 84% of total (about 334 mrem/year) | ||||||
Inhaled radon | 200 | 50 | ||||
Ingested with food | 40 | 10 | ||||
Cosmic radiation | 27 | 7 | ||||
Terrestrial radiation | 28 | 7 | ||||
Internal body | 39 | 10 | ||||
Man-made sources 16% of total (about 65 mrem/year) | ||||||
Medical x-rays | 39 | 10 | ||||
Nuclear medicine | 14 | 4 | ||||
Consumer products | 9 | 2 | ||||
Occupational exposure | 0.9 | 0.2 | ||||
Weapons testing fallout | <0.9 | <0.2 | ||||
Nuclear fuel cycle | 0.4 | 0.1 | ||||
Miscellaneous | 0.4 | 0.1 |