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H-3 beta shielding — range and bremsstrahlung

Tritium

H-3 · Hydrogen, Z = 1, A = 3

At 3.56e+14 Bq/g — 9.62e+3 Ci/g — a gigabecquerel of H-3 amounts to 2.81 µg, which is why activity rather than mass is how anyone states the quantity. Tritium decays by beta-minus decay with a half-life of 12.32 years, falling to 94.53% of today's activity in a year and 10.53% in forty years.

The beta endpoint is 0.0186 MeV, mean 0.00568 MeV over 1 branch. That endpoint stops in 0.00496 mm of acrylic or 0.00234 mm of glass. Of the beta energy, 3.9e-3% turns into X-rays in acrylic and 0.05% in lead.

Decay is the only handle: a year leaves 94.53% of today's activity and forty years leaves 10.53%, with ten half-lives at 123 years and a mean life of 17.8 years per atom.

Half-life, specific activity and beta endpoint

Half-life12.32 years (3.888e+8 s)
Decay modebeta-minus decay
Specific activity3.56e+14 Bq/g (9.62e+3 Ci/g)
Beta endpoint / mean0.0186 MeV / 0.00568 MeV

0.00496 mm of acrylic stops the 0.0186 MeV endpoint

Katz–Penfold fit to the 0.0186 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)
acrylic0.00496
aluminum0.00217
water0.00585
glass0.00234
Shield materialFraction of beta energy converted to X-rays
acrylic (Z ≈ 6)0.00%
lead (Z = 82)0.05%

Activity over decades and centuries

Ten half-lives is 123 years, which puts decay storage out of reach: 10.53% survives forty years. The mean life 1/λ, the quantity that enters an integrated dose, is 17.8 years.

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 activity40.9 years
Time to fall to 1 %81.9 years
Time to fall to 0.1 %123 years

Limits of these range figures

Beta and decay calculators for H-3

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