Radium-226
Ra-226 · Radium, Z = 88, A = 226
A gigabecquerel of Ra-226 is 27.3 mg of material, which follows from a specific activity of 3.66e+10 Bq/g (0.989 Ci/g). Radium-226 decays by alpha decay with a half-life of 1600 years; forty years leaves 98.28% of today's activity and ten thousand years leaves 1.31%.
The air kerma rate constant recorded for Ra-226 is 0.000879 mGy·m²/(GBq·h). 1 GBq at 1 m reads 0.000879 mGy/h, and 1 Ci at the same distance 0.0325 mGy/h — for that emission alone. No ranking against the other emitters here is drawn: for most of them the constant is the whole field, and for Ra-226 it is not.
7 lines clear the 20 keV cutoff, but one of them carries 90% of the dose rate. The leading one is 186.2 keV at 91.1% of the total — its emission probability is 3.565%, which is also the highest.
For Ra-226's own photons, 0.473 mm of lead halves the air kerma rate, 5.07 mm if the material is steel, and 1.65 mm of lead takes it to a tenth. What thickness the source in front of you needs is a question about its chain, not about this line list.
These photon figures are Ra-226's own. What it decays into is not in this dataset, so nothing below Ra-226 is counted here. A source left sealed long enough for the chain to build up reads higher than this — how much higher is outside what this page can compute.
Alpha emission is led by 4.784 MeV at 94.07%, one of 2 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-life | 1600 years (5.049e+10 s) |
| Decay mode | alpha decay |
| Specific activity | 3.66e+10 Bq/g (0.989 Ci/g) |
| Air kerma rate constant Γ (δ = 20 keV) | 0.000879 mGy·m²/(GBq·h) |
| Dose rate, 1 GBq at 1 m | 0.000879 mGy/h |
| Dose rate, 1 Ci at 1 m | 0.0325 mGy/h |
| Kerma-weighted mean photon energy | 177.8 keV |
186 keV carries 91% of the dose rate
1 further line below the 20 keV cutoff, the highest at 14.09 keV and 0.783% emission probability in all, is excluded here and from Γ. Why the two columns rank differently.
| Energy (keV) | Emission probability (%) | Share of dose rate (%) |
|---|---|---|
| 186.21 | 3.565 | 91.12 |
| 83.79 | 0.31774 | 3.32 |
| 81.07 | 0.19261 | 1.96 |
| 96.05 | 0.14545 | 1.71 |
| 94.88 | 0.11019 | 1.28 |
| 97.53 | 0.03526 | 0.42 |
| 262.27 | 0.005 | 0.19 |
0.473 mm of lead halves this spectrum
Solved numerically across all 7 lines, narrow beam. Why not one representative energy.
| Material | HVL (mm) | TVL (mm) | TVL / HVL |
|---|---|---|---|
| lead | 0.473 | 1.65 | 3.49 |
| tungsten | 0.337 | 1.23 | 3.65 |
| iron | 5.07 | 17.9 | 3.53 |
| copper | 4.08 | 14.5 | 3.56 |
| concrete | 22.1 | 74.1 | 3.35 |
| water | 48.4 | 161 | 3.33 |
| aluminum | 19.7 | 66.0 | 3.36 |
A single energy would give 3.32. What a spread of energies does instead.
2 alpha lines, strongest 4.784 MeV
2 recorded lines from 4.601 to 4.784 MeV, the strongest 4.784 MeV at 94.07% of 100.0% total alpha emission.
| Energy (MeV) | Emission probability (%) |
|---|---|
| 4.7843 | 94.07 |
| 4.6010 | 5.93 |
Activity over millennia
Ten half-lives is 16,000 years. On any timescale a facility can be planned over the activity is constant — 98.28% is left after forty years — and the mean life 1/λ is 2,308 years.
| Elapsed | Fraction remaining |
|---|---|
| 1 half-life | 50.0 % |
| 2 half-lives | 25.0 % |
| 5 half-lives | 3.13 % |
| 10 half-lives | 0.0977 % |
| Time to fall to 10 % of today's activity | 5,315 years |
| Time to fall to 1 % | 10,630 years |
| Time to fall to 0.1 % | 15,945 years |
Limits — intake, not external dose
- 0.000879 mGy/h at a metre — bare point source, no capsule, no self-absorption.
- 0.473 mm of lead halves this spectrum, narrow beam, scatter not added back.
- Γ excludes 1 line under 20 keV, carrying 0.783% of all emissions.
- Alpha reaches nothing through skin — Ra-226 is an intake problem, not an external one.
- What every sheet leaves out, internal dose included.
Gamma and decay calculators for Ra-226
Other Radium nuclides: Ra-223, Ra-224, Ra-228
Computed from the IAEA Nuclear Data Section — Livechart API (ENSDF) and the NIST X-Ray Mass Attenuation Coefficients. Derivations and citations.