Why might 123 I be preferred for imaging over 131 I? (a) The atomic mass of 123
Question:
Why might 123I be preferred for imaging over 131I?
(a) The atomic mass of 123I is smaller, so the 123I particles travel farther through tissue.
(b) Because 123I emits only gamma-ray photons, the radiation dose to the body is lower with that isotope.
(c) The beta particles emitted by 131I can leave the body, whereas the gamma ray photons emitted by 123I cannot.
(d) 123I is radioactive, whereas 131I is not.
Iodine in the body is preferentially taken up by the thyroid gland. Therefore, radioactive iodine in small doses is used to image the thyroid and in large doses is used to kill thyroid cells to treat some types of cancer or thyroid disease. The iodine isotopes used have relatively short half-lives, so they must be produced in a nuclear reactor or accelerator. One isotope frequently used for imaging is 123I; it has a half-life of 13.2 h and emits a 0.16-MeV gamma-ray photon. One method of producing 123I is in the nuclear reaction 123Te + p → 123I + n. The atomic masses relevant to this reaction are 123Te, 122.904270 u; 123I, 122.905589 u; n, 1.008665 u; and 1H, 1.007825 u.
The iodine isotope commonly used for treatment of disease is 131I, which is produced by irradiating 130Te in a nuclear reactor to form 131Te. The 131Te then decays to 131I. 131I undergoes b- decay with a half-life of 8.04 d, emitting electrons with energies up to 0.61 MeV and gamma ray photons of energy 0.36 MeV. A typical thyroid cancer treatment might involve administration of 3.7 GBq of 131I.
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University Physics with Modern Physics
ISBN: 978-0133977981
14th edition
Authors: Hugh D. Young, Roger A. Freedman