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Bi-210 beta shielding — range and bremsstrahlung

Bismuth-210

Bi-210 · Bismuth, Z = 83, A = 210

At 4.59e+15 Bq/g — 1.24e+5 Ci/g — a gigabecquerel of Bi-210 amounts to 218 ng, which is why activity rather than mass is how anyone states the quantity. Bismuth-210 decays by beta-minus decay with a half-life of 5.012 days, falling to 37.98% of today's activity in a week and 3.4e-4% in three months.

The beta endpoint is 1.16 MeV, mean 0.389 MeV over 1 branch. That endpoint stops in 4.21 mm of acrylic or 1.99 mm of glass. Of the beta energy, 0.24% turns into X-rays in acrylic and 3.33% in lead.

Decay is the only handle: a week leaves 37.98% of today's activity and three months leaves 3.4e-4%, with ten half-lives at 50.1 days and a mean life of 7.23 days per atom.

Half-life, specific activity and beta endpoint

Half-life5.012 days (4.330e+5 s)
Decay modebeta-minus decay
Specific activity4.59e+15 Bq/g (1.24e+5 Ci/g)
Beta endpoint / mean1.16 MeV / 0.389 MeV

4.21 mm of acrylic stops the 1.16 MeV endpoint

Katz–Penfold fit to the 1.16 MeV endpoint — ±10%, and a stopping thickness rather than an attenuation length. Why the material matters more than the thickness.

AbsorberRange for the endpoint (mm)
acrylic4.21
aluminum1.84
water4.97
glass1.99
Shield materialFraction of beta energy converted to X-rays
acrylic (Z ≈ 6)0.24%
lead (Z = 82)3.33%

Activity over months and years

Ten half-lives is 50.1 days — a storage problem rather than a disposal one, with 1.2e-20% of today's activity still there after a year. The mean life 1/λ is 7.23 days.

ElapsedFraction remaining
1 half-life50.0 %
2 half-lives25.0 %
5 half-lives3.13 %
10 half-lives0.0977 %
Time to fall to 10 % of today's activity16.6 days
Time to fall to 1 %33.3 days
Time to fall to 0.1 %49.9 days

Limits of these range figures

Beta and decay calculators for Bi-210

Computed from the IAEA Nuclear Data Section — Livechart API (ENSDF) and the NIST X-Ray Mass Attenuation Coefficients. Derivations and citations.