ALARA exposure planner
ALARA - as low as reasonably achievable - is not a slogan, it is an arithmetic exercise done before the source leaves the pot. Three multiplicative factors set the dose anyone receives, and each can be traded against the others: activity (which decays with time), distance (inverse square), and shielding (exponential). Multiply them together and the field at any position is D = Gamma x A0 x 2^(-dt/T_half) / d^2 x 2^(-x/HVL).
Seeing the three terms side by side is what makes the planning decision obvious. Distance is free and works in every direction, so it is always the first lever - moving from 5 m to 10 m removes 75 percent of the dose at no cost but time. Shielding is expensive and heavy but works where distance is unavailable, such as an adjacent occupied room. Decay works for you slowly, but it also means a source nearing replacement gives a smaller barrier and a longer exposure at the same time.
Dose is then simply rate times occupancy. A planner that shows the dose for the actual time a technician stands at the barrier, rather than a worst-case hour, is what turns a barrier calculation into a defensible dose assessment. The complementary figure is stay time: how long the position can be occupied before a chosen budget is spent.
Everything here is a free-air point-source calculation with narrow-beam attenuation. Scatter adds to the result and build-up in a thick shield adds more. Use it to plan the layout and predict the survey, never to replace it.
A = A0 x 2^(-dt / T_half) D_unshielded = 8760 x Gamma x A / d^2 (uSv/h) D_shielded = D_unshielded x B x 2^(-x / HVL) Dose = D_shielded x occupancy Barrier radius = sqrt(8760 x Gamma x A / D_limit)
- Free-air point source. At the default B = 1 the shield term is narrow-beam - set B above 1 to include scatter build-up in a thick shield.
- The barrier radius shown is for the unshielded source in the open directions.
- Plan with this, prove with a survey meter, record with an electronic personal dosimeter.
Reference: IAEA GSR Part 3 (2014); ICRP Publication 103 (2007); NCRP Report No. 49


