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Calculators / Dose and shielding

Co-60 shielding: half-value layers and required thickness

Co-60’s two gammas at 1173 and 1332 keV make it the reference hard-to-shield source. Its unshielded rate is 13.1 mSv/h H*(10) per curie at 1 m. Buildup matters here: a broad-beam half-value layer is thicker than the textbook narrow-beam one, and the gap grows with depth.

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1 Ci @ 1 m, H*(10)
13.1 mSv/h
1 Ci @ 1 m, EXPOSURE
1.29 R/h
LEAD HVL (BROAD)
1.56 cm
CONCRETE TVL (BROAD)
30.5 cm

Half- and tenth-value layers

MATERIALHVL NARROWHVL BROADTVL NARROWTVL BROAD
Lead1.03 cm1.56 cm3.44 cm4.65 cm
Tungsten0.642 cm1.02 cm2.14 cm2.98 cm
Steel (iron)1.65 cm3.58 cm5.48 cm9.24 cm
Concrete5.2 cm12.4 cm17.3 cm30.5 cm
Water11 cm28.5 cm36.5 cm67.4 cm

Narrow beam counts only unscattered photons, e−μx. Broad beam adds the scattered ones through the buildup factor B, and is the one that matters for a shield. Because B grows with depth, a TVL is more than 3.32 HVLs.

The buildup here is the ANSI/ANS-6.4.3 point-isotropic factor for each material, an infinite-medium value: it overstates the scatter that reaches a point behind a finite wall. A slab Monte Carlo in the app’s audit puts the true dose 1 m behind 30 cm of concrete about 1.4× lower, and behind 10 cm of lead about 1.2× lower, so a design based on these values errs on the thick side. The values are also first layers, from zero thickness; deeper layers are thinner.

Worked examples

Lead. A 1 Ci (37 GBq) source read at 1 m:

to 25 µSv/h   11.6 cm of lead
to 2.5 µSv/h  15.5 cm of lead

Concrete. The same source, with the wall’s far face at 3 m, needs 68.3 cm of ordinary concrete for 2.5 µSv/h.

Both thicknesses are solved in the app’s Shield mode and checked by putting the answer back through the dose calculation.

Assumptions

Sources

Numbers on this page computed by the physics code of Nuclear Toolkit 1.4.1, the same code as the app. How it is checked.

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