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Am-241 shielding — lead half-value layer and dose rate

Americium-241

Am-241 · Americium, Z = 95, A = 241

A gigabecquerel of Am-241 is 7.88 mg of material, which follows from a specific activity of 1.27e+11 Bq/g (3.43 Ci/g). Americium-241 decays by alpha decay with a half-life of 432.6 years; forty years leaves 93.79% of today's activity and ten thousand years leaves 1.1e-5%.

The air kerma rate constant is small — 0.00369 mGy·m²/(GBq·h), 21× less than Cs-137 and 83× less than Co-60, ranking 78 of 96 by Γ — near the bottom of the photon emitters, but above the cutoff, which 51 nuclides in this dataset are not. 1 GBq at 1 m reads 0.00369 mGy/h, and 1 Ci at the same distance 0.137 mGy/h. It takes 5.41 GBq at a metre to reach 20 µSv/h from the photons alone.

14 lines clear the 20 keV cutoff, but 2 of them carry 90% of the dose rate. The leading one is 59.5 keV at 81.8% of the total — its emission probability is 35.9%, which is also the highest.

Shielding barely arises: 0.0865 mm of lead halves the air kerma rate and 0.362 mm takes it to a tenth, thicknesses a source capsule is likely to exceed on its own. Steel does the halving in 0.517 mm. At 1 GBq and a metre it is already under 20 µSv/h with nothing in the way. The tenth-value layer runs 4.2 times the half-value layer, not the 3.32 a single energy would give.

Alpha emission is led by 5.486 MeV at 84.8%, one of 7 recorded lines. None of it reaches through skin, so the alpha is an intake hazard rather than an external one — the photon figures above are the separate question.

Half-life, specific activity and dose rate

Half-life432.6 years (1.365e+10 s)
Decay modealpha decay
Specific activity1.27e+11 Bq/g (3.43 Ci/g)
Air kerma rate constant Γ (δ = 20 keV)0.00369 mGy·m²/(GBq·h)
Dose rate, 1 GBq at 1 m0.00369 mGy/h
Dose rate, 1 Ci at 1 m0.137 mGy/h
Kerma-weighted mean photon energy53.71 keV

59.5 keV carries 82% of the dose rate

1 further line below the 20 keV cutoff, the highest at 17.14 keV and 36.6% emission probability in all, is excluded here and from Γ. Why the two columns rank differently.

Energy (keV)Emission probability (%)Share of dose rate (%)
59.5435.981.80
26.342.2717.07
33.200.1260.60
43.420.0730.22
32.180.01740.09
102.980.01950.06
98.970.02030.06
55.560.01810.04
42.700.00550.02
125.300.004080.02
57.850.00520.01
69.760.00290.01
101.070.001850.01
97.080.001160.00

0.0865 mm of lead halves this spectrum

Solved numerically across all 14 lines, narrow beam. Why not one representative energy.

MaterialHVL (mm)TVL (mm)TVL / HVL
lead0.08650.3624.18
tungsten0.06870.2884.19
iron0.5172.184.21
copper0.3441.454.22
concrete8.4934.14.01
water28.71033.58
aluminum6.8227.84.07

A single energy would give 3.32. What a spread of energies does instead.

7 alpha lines, strongest 5.486 MeV

7 recorded lines from 5.322 to 5.545 MeV, the strongest 5.486 MeV at 84.8% of 100.2% total alpha emission.

Energy (MeV)Emission probability (%)
5.485684.8
5.442813.1
5.38801.66
5.54450.37
5.51150.225
5.46900.04
5.32200.015

Activity over millennia

Ten half-lives is 4,326 years, which puts decay storage out of reach: 93.79% survives forty years. The mean life 1/λ, the quantity that enters an integrated dose, is 624 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 activity1,437 years
Time to fall to 1 %2,874 years
Time to fall to 0.1 %4,311 years

Limits — intake, not external dose

Gamma and decay calculators for Am-241

Other Americium nuclides: Am-243

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