TABLE 1

Mathematic Notations and Definitions

NotationDefinition
B2The transmission factor for radiation emanating from compartment 2 (thyroid)
d1The distance (m) to a bystander from the patient’s skin at the extrathyroidal source
d2The distance (m) to a bystander from the patient’s skin at the thyroid
Δd1The depth in the patient (m) of the extrathyroidal line source
Δd2The depth in the patient (m) of the thyroidal point source
Embedded ImageThe fraction of administered isotope initially partitioned into compartment 1
Embedded ImageThe fraction of administered isotope initially partitioned into compartment 2
giThe perpendicular distance from the cylinder’s ith line source to the dose point
ΔgiThe perpendicular distance from the cylinder’s ith line source to the cylinder’s surface in the direction of the dose point
HVLThe broad-beam half-value layer in water (m) of 131I’s 364-keV photon (the value 0.1 m is used, reference (9))
Embedded ImageThe air kerma rate at the position of a bystander resulting from patient emanations
Embedded ImageThe total air kerma at the position of a bystander beginning at a start time ts
lVariable of integration, distance from midpoint of a line source to line source element dl
LThe length (m) of the line source
Embedded ImageThe amount of isotope remaining in metabolic compartment 1 (extrathyroid) at time t
Embedded ImageThe amount of isotope remaining in metabolic compartment 2 (thyroid) at time t
Embedded ImageThe amount of isotope in the bladder at time t when the previous urination was at time T
Embedded ImageThe amount of isotope remaining in the patient at time t (parallel model)
Embedded ImageThe amount of isotope initially administered
Embedded ImageThe effective half-life for the radioisotope leaving metabolic compartment 1
Embedded ImageThe effective half-life for the radioisotope leaving metabolic compartment 2
TocThe occupancy factor, that is, the average fraction of time that a specific bystander is present at a specified location
tsThe time that a family member or other bystander begins exposure to the patient’s radiation field
ΓThe air kerma rate constant (mGy/h/MBq at 1 m) for the radioisotope (the value 5.1613E−5 is used for 131I)
Embedded ImageThe rate constant for the radioisotope leaving a metabolic compartment by nuclear decay
Embedded ImageThe rate constant for the isotope leaving metabolic compartment 1 by biologic processes
Embedded ImageThe rate constant for the isotope leaving metabolic compartment 2 by biologic processes
Embedded ImageThe effective rate constant for the isotope leaving metabolic compartment 1
Embedded ImageThe effective rate constant for the isotope leaving metabolic compartment 2
Embedded ImageThe relationship between rate constant and half-life, where ln(2) is the natural log of 2