Validation
Run 2026-09-29 against version 1.4.1
Every number in the tables below was computed by the app’s own physics
code — the same code the iOS, Android and web apps run — and
compared with a value from outside it: a handbook table, a textbook
identity, or an independent calculation written separately for the test. A
check outside its tolerance fails the test suite, and this page is only
regenerated when none does.
- CHECKS
- 174
- OUTSIDE TOLERANCE
- 0
- AREAS
- 8decay to reactor physics
- VERSION
- 1.4.12026-09-29
How to read the tables
- REFERENCE
-
Where the comparison value comes from. A handbook, ENSDF, CIAAW or a
textbook appendix is a published value. “Definition”,
“round trip”, “RK4” and “by hand” are
independent calculations: they show that the equations are solved
correctly, not that the input data is right. The published-value rows
cover the data.
- TOLERANCE
-
How precisely the reference itself is quoted, fixed before the check
ran — not how close the app happened to land. A rule of thumb such
as Co-60 at 1.32 R/h per curie at 1 m gets ±6 %;
an exact definition gets a millionth of a percent.
- NOT CLAIMED
-
Conformance to NQA-1, 10 CFR 50 Appendix B or any software
quality programme. If your work requires qualified software, use this
app as a cross-check, not as the system of record.
Decay and specific activity 13
Closed-form identities
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| lambda = ln2/T½ | 7.3020 × 10⁻¹⁰ | 7.3020 × 10⁻¹⁰ | < 0.01 % | ± 1e-6 % | definition |
| A(1 T½)/A₀ | 0.5 | 0.5 | < 0.01 % | ± 1e-6 % | definition |
| A(10 T½)/A₀ | 9.7656 × 10⁻⁴ | 9.7656 × 10⁻⁴ | < 0.01 % | ± 1e-6 % | definition |
| t(1%) in half-lives | 6.64386 | 6.64386 | < 0.01 % | ± 1e-4 % | definition |
| A(−1 T½) back-decay | 2 | 2 | < 0.01 % | ± 1e-6 % | inverse decay |
Specific activity vs published Ci/g
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| specific activity Co-60 (Ci/g) | 1131.61 | 1131 | +0.05 % | ± 3 % | handbook |
| specific activity Cs-137 (Ci/g) | 86.8113 | 87 | −0.22 % | ± 3 % | handbook |
| specific activity Ra-226 (Ci/g) | 0.988559 | 0.988 | +0.06 % | ± 3 % | handbook |
| specific activity Sr-90 (Ci/g) | 137.542 | 138 | −0.33 % | ± 5 % | handbook |
| specific activity H-3 (Ci/g) | 9621.24 | 9650 | −0.30 % | ± 5 % | handbook |
| specific activity Pu-239 (Ci/g) | 0.0620283 | 0.0621 | −0.12 % | ± 5 % | handbook |
| specific activity U-235 (Ci/g) | 2.1605 × 10⁻⁶ | 2.1600 × 10⁻⁶ | +0.02 % | ± 5 % | handbook |
| specific activity I-131 (Ci/g) | 1.2429 × 10⁵ | 1.2400 × 10⁵ | +0.24 % | ± 5 % | handbook |
Decay chains 4
Ra-226 chain reaches secular equilibrium in one year
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| secular equilibrium Rn-222/Ra-226 | 1.00001 | 1 | < 0.01 % | ± 2 % | T½(daughter) ≪ T½(parent) |
| secular equilibrium Pb-214/Ra-226 | 0.999807 | 1 | −0.02 % | ± 2 % | T½(daughter) ≪ T½(parent) |
| secular equilibrium Bi-214/Ra-226 | 0.999807 | 1 | −0.02 % | ± 2 % | T½(daughter) ≪ T½(parent) |
Ba-140 → La-140 reaches TRANSIENT equilibrium, not secular
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| La-140/Ba-140 activity at 30 d | 1.15158 | 1.15157 | < 0.01 % | ± 1 % | λ_d/(λ_d−λ_p) |
Gamma dose and shielding 47
Gamma constants vs published R/h per Ci at 1 m
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| Γ Co-60 (R/h per Ci @1 m) | 1.29091 | 1.32 | −2.20 % | ± 6 % | handbook |
| Γ Cs-137 (R/h per Ci @1 m) | 0.325846 | 0.33 | −1.26 % | ± 6 % | handbook |
| Γ Ir-192 (R/h per Ci @1 m) | 0.50333 | 0.48 | +4.86 % | ± 12 % | handbook |
| Γ Na-22 (R/h per Ci @1 m) | 1.18349 | 1.2 | −1.38 % | ± 8 % | handbook |
| Γ I-131 (R/h per Ci @1 m) | 0.220196 | 0.22 | +0.09 % | ± 15 % | handbook |
| Γ Mn-54 (R/h per Ci @1 m) | 0.463421 | 0.47 | −1.40 % | ± 8 % | handbook |
| Γ Au-198 (R/h per Ci @1 m) | 0.238276 | 0.23 | +3.60 % | ± 20 % | handbook |
| Γ Zn-65 (R/h per Ci @1 m) | 0.303571 | 0.27 | +12.43 % | ± 20 % | handbook |
Geometry, linearity, and the HVL/TVL definitions
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| inverse square 1 m → 2 m | 4 | 4 | < 0.01 % | ± 0.01 % | 1/r² |
| linearity in activity | 2 | 2 | < 0.01 % | ± 1e-6 % | rate ∝ A |
| spectrum HVL halves the rate | 0.5 | 0.5 | < 0.01 % | ± 1 % | definition |
| spectrum TVL → 10 % of rate | 0.1 | 0.1 | < 0.01 % | ± 1 % | definition |
Narrow-beam HVL equals ln2/µ from the shipped NIST table
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| Cs-137 narrow HVL Pb (cm) | 0.549926 | 0.5499 | < 0.01 % | ± 1 % | ln2/µ @662 keV |
| Co-60 narrow HVL Pb (cm) | 1.03932 | 1.0367 | +0.25 % | ± 1 % | ln2/µ @1.25 MeV |
| Buildup ≥ 1 and rising with depth (Pb, 1 MeV) | B = 1.367 at 1 mfp, 2.444 at 5 mfp | pass | — | physical requirement |
H*(10)/Ka lies in the ICRP 74 band
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| H*(10)/Ka for Cs-137 | ratio 1.2035, band 1.00–1.35 | pass | — | ICRP 74 Table A.21 |
| H*(10)/Ka for Co-60 | ratio 1.1588, band 1.00–1.35 | pass | — | ICRP 74 Table A.21 |
| H*(10)/Ka for Ir-192 | ratio 1.1724, band 1.00–1.35 | pass | — | ICRP 74 Table A.21 |
Solvers reproduce their own targets (round trips)
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| shield Ir-192 in lead: rate at answer | 2.5000 × 10⁻⁶ | 2.5000 × 10⁻⁶ | < 0.01 % | ± 1e-3 % | round trip |
| shield Co-60 in concrete: rate at answer | 2.5000 × 10⁻⁶ | 2.5000 × 10⁻⁶ | < 0.01 % | ± 1e-3 % | round trip |
| shield Pb-212+ in lead: rate at answer | 2.5000 × 10⁻⁶ | 2.5000 × 10⁻⁶ | < 0.01 % | ± 1e-3 % | round trip |
| shield Ba-140+ in iron: rate at answer | 2.5000 × 10⁻⁶ | 2.5000 × 10⁻⁶ | < 0.01 % | ± 1e-3 % | round trip |
| distance Co-60: rate at answer | 1.0000 × 10⁻⁴ | 1.0000 × 10⁻⁴ | < 0.01 % | ± 1e-3 % | round trip |
| distance Tc-99m: rate at answer | 1.0000 × 10⁻⁴ | 1.0000 × 10⁻⁴ | < 0.01 % | ± 1e-3 % | round trip |
| distance F-18: rate at answer | 1.0000 × 10⁻⁴ | 1.0000 × 10⁻⁴ | < 0.01 % | ± 1e-3 % | round trip |
| Co-60 concrete: transmission at HVL | 0.5 | 0.5 | < 0.01 % | ± 0.5 % | definition |
| Co-60 concrete: transmission at TVL | 0.1 | 0.1 | < 0.01 % | ± 0.5 % | definition |
| Ir-192 tungsten: transmission at HVL | 0.5 | 0.5 | < 0.01 % | ± 0.5 % | definition |
| Ir-192 tungsten: transmission at TVL | 0.1 | 0.1 | < 0.01 % | ± 0.5 % | definition |
+progeny entries equal their members summed by hand
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| Γ Pb-212+ = Pb-212 + Bi-212 + Tl-208 | 0.00654472 | 0.00654953 | −0.07 % | ± 0.3 % | ENSDF, by hand |
| Γ Ba-140+ = Ba-140 + La-140 | 0.0127361 | 0.0127358 | < 0.01 % | ± 0.3 % | ENSDF, by hand |
| Γ Mo-99+ = Mo-99 + 0.876 Tc-99m | 0.00125906 | 0.00125906 | < 0.01 % | ± 0.3 % | ENSDF, by hand |
ANS-6.4.3 buildup and the coherent-free μ it requires
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| B lead, 1 MeV, 4 mfp | 2.20577 | 2.21 | −0.19 % | ± 3 % | ANS-6.4.3 Table 3 |
| B lead, 0.5 MeV, 10 mfp | 2.08471 | 2.1 | −0.73 % | ± 3 % | ANS-6.4.3 Table 3 |
| B water, 1 MeV, 10 mfp | 26.4353 | 26.1 | +1.28 % | ± 3 % | ANS-6.4.3 Table 3 |
| B water, 0.5 MeV, 5 mfp | 18.1154 | 18.4 | −1.55 % | ± 3 % | ANS-6.4.3 Table 3 |
| B concrete, 1 MeV, 10 mfp | 20.7183 | 20.7 | +0.09 % | ± 3 % | ANS-6.4.3 Table 3 |
| B iron, 1 MeV, 10 mfp | 15.733 | 15.8 | −0.42 % | ± 3 % | ANS-6.4.3 Table 3 |
| B iron, 0.5 MeV, 5 mfp | 7.70649 | 7.68 | +0.34 % | ± 3 % | ANS-6.4.3 Table 3 |
| B aluminum, 1 MeV, 10 mfp | 21.0423 | 21 | +0.20 % | ± 3 % | ANS-6.4.3 Table 3 |
| coherent share of μ, lead, 662 keV (%) | 6.03338 | 5.99455 | +0.65 % | ± 5 % | NIST XCOM |
Behind a wall the point kernel stays at or above a slab Monte Carlo
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| Cs-137, 20 cm of concrete, 1 m behind: app at or above slab Monte Carlo | app/MC = 1.55 (transmission 1.84e-1 vs 1.19e-1) | pass | — | Klein–Nishina slab Monte Carlo |
| Co-60, 30 cm of concrete, 1 m behind: app at or above slab Monte Carlo | app/MC = 1.36 (transmission 1.05e-1 vs 7.77e-2) | pass | — | Klein–Nishina slab Monte Carlo |
| Cs-137, 40 cm of water, 1 m behind: app at or above slab Monte Carlo | app/MC = 1.66 (transmission 2.64e-1 vs 1.58e-1) | pass | — | Klein–Nishina slab Monte Carlo |
| Cs-137, 5 cm of lead, 1 m behind: app at or above slab Monte Carlo | app/MC = 1.13 (transmission 5.53e-3 vs 4.88e-3) | pass | — | Klein–Nishina slab Monte Carlo |
| Ir-192, 2 cm of lead, 1 m behind: app at or above slab Monte Carlo | app/MC = 1.08 (transmission 2.74e-2 vs 2.55e-2) | pass | — | Klein–Nishina slab Monte Carlo |
| Co-60, 10 cm of lead, 1 m behind: app at or above slab Monte Carlo | app/MC = 1.19 (transmission 4.82e-3 vs 4.05e-3) | pass | — | Klein–Nishina slab Monte Carlo |
Metastable isomers 20
Decay law and published half-lives
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| isomer T½ Tc-99m (s) | 21625.9 | 21625.9 | < 0.01 % | ± 3 % | IAEA/ENSDF |
| isomer T½ Ba-137m (s) | 153.12 | 153.12 | < 0.01 % | ± 3 % | IAEA/ENSDF |
| isomer T½ Ag-110m (s) | 2.1585 × 10⁷ | 2.1585 × 10⁷ | < 0.01 % | ± 3 % | IAEA/ENSDF |
| isomer T½ In-113m (s) | 5968.56 | 5968.56 | < 0.01 % | ± 3 % | IAEA/ENSDF |
| isomer T½ Kr-83m (s) | 6588 | 6588 | < 0.01 % | ± 3 % | IAEA/ENSDF |
| isomer T½ Sr-87m (s) | 10134 | 10134 | < 0.01 % | ± 5 % | IAEA/ENSDF |
| Tc-99m A(1 T½)/A₀ | 0.5 | 0.5 | < 0.01 % | ± 1e-6 % | definition |
| Ba-137m excitation = 661.66 keV line | 661.659 | 661.657 | < 0.01 % | ± 0.1 % | ENSDF |
Branching ratios are physical
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| isomers reporting 0 % for every branch | 0 | 0 | exact | exact | conversion rule |
Delayed channels are not counted as competing branches
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| Rb-98m primary branches | 100 | 100 | < 0.01 % | ± 0.01 % | NUBASE2020 §2.4 |
| Rb-98m β-delayed channels held apart | delayed: B-2N,B-N | pass | — | NUBASE2020 §2.4 |
| delayed channels leaked into decayModes | 0 | 0 | exact | exact | NUBASE2020 §2.4 |
Isomer gamma sources are reachable in the Dose tab
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| Tc-99m selectable as a dose source | 4 lines | pass | — | IAEA decay_rads |
| Ba-137m selectable as a dose source | 6 lines | pass | — | IAEA decay_rads |
| Ag-110m selectable as a dose source | 35 lines | pass | — | IAEA decay_rads |
| Xe-135m selectable as a dose source | 6 lines | pass | — | IAEA decay_rads |
| Kr-85m selectable as a dose source | 7 lines | pass | — | IAEA decay_rads |
| Tc-99m dominant γ (keV) | 140.511 | 140.511 | < 0.01 % | ± 0.1 % | ENSDF |
| Tc-99m dominant γ intensity (%) | 89 | 89 | < 0.01 % | ± 5 % | ENSDF |
| Ba-137m dominant γ (keV) | 661.657 | 661.657 | < 0.01 % | ± 0.1 % | ENSDF |
Neutron cross sections and activation 30
Literature anchors and internal identities
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| σ₀ B-10 (n,α) (b) | 3837 | 3837 | < 0.01 % | ± 1 % | Lamarsh App. II |
| σ₀ Li-6 (n,α) (b) | 940 | 940 | < 0.01 % | ± 1 % | Lamarsh App. II |
| σ₀ He-3 (n,p) (b) | 5330 | 5330 | < 0.01 % | ± 1 % | Lamarsh App. II |
| σ₀ H-1 (n,γ) (b) | 0.3326 | 0.3326 | < 0.01 % | ± 1 % | Lamarsh App. II |
| σ₀ Cd-113 (n,γ) (b) | 20600 | 20600 | < 0.01 % | ± 1 % | Mughabghab 2006 |
| σ₀ Gd-157 (n,γ) (b) | 2.5400 × 10⁵ | 2.5400 × 10⁵ | < 0.01 % | ± 1 % | Mughabghab 2006 |
| σ₀ Sm-149 (n,γ) (b) | 40140 | 40140 | < 0.01 % | ± 1 % | D&H Ch. 15 |
| σ₀ U-235 (n,f) (b) | 582 | 582 | < 0.01 % | ± 1 % | Lamarsh App. II |
| σ₀ U-238 (n,γ) (b) | 2.68 | 2.68 | < 0.01 % | ± 1 % | Lamarsh App. II |
| σ₀ Pu-239 (n,f) (b) | 748 | 748 | < 0.01 % | ± 1 % | Lamarsh App. II |
| σ₀ Au-197 (n,γ) (b) | 98.65 | 98.65 | < 0.01 % | ± 1 % | Mughabghab 2006 |
| U-235 σ_f+σ_γ = σ_a (b) | 681 | 681 | < 0.01 % | ± 0.01 % | definition |
| Pu-239 σ_f+σ_γ = σ_a (b) | 1017 | 1017 | < 0.01 % | ± 0.01 % | definition |
| σ_Xe cross_sections vs xenon.ts (b) | 2.6500 × 10⁶ | 2.6500 × 10⁶ | < 0.01 % | ± 0.01 % | internal consistency |
| U-235 α = σ_γ/σ_f | 0.170103 | 0.169 | +0.65 % | ± 3 % | Lamarsh §4 |
| U-235 η = ν·σ_f/σ_a | 2.06819 | 2.068 | +0.01 % | ± 2 % | Lamarsh §4 (η ≈ 2.07) |
| H weighted sigma_a (b) | 0.332552 | 0.3326 | −0.01 % | ± 3 % | Lamarsh & Baratta 3rd ed., App. II |
| C weighted sigma_a (b) | 0.0035071 | 0.0035 | +0.20 % | ± 3 % | Lamarsh & Baratta 3rd ed., App. II |
| N weighted sigma_a (b) | 1.89777 | 1.9 | −0.12 % | ± 3 % | Lamarsh & Baratta 3rd ed., App. II |
| Fe weighted sigma_a (b) | 2.5641 | 2.56 | +0.16 % | ± 3 % | Mughabghab (2006), elemental value |
| Pb weighted sigma_a (b) | 0.174208 | 0.171 | +1.88 % | ± 3 % | Mughabghab (2006), elemental value |
Høgdahl rate for gold, by hand
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| Au saturation, thermal 1e12 | 3.0162 × 10¹¹ | 3.0162 × 10¹¹ | < 0.01 % | ± 1 % | Mughabghab σ₀ |
| Au saturation, φₑ = φ_th/30 | 4.5958 × 10¹¹ | 4.5958 × 10¹¹ | < 0.01 % | ± 1.5 % | Høgdahl, Mughabghab I₀ |
IRDFF-II averages and an independent fission spectrum
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| σ̄ Fe-54(n,p), U-235 fission (mb) | 76.635 | 76.66 | −0.03 % | ± 1 % | IAEA IRDFF-II |
| σ̄ Ni-58(n,p), U-235 fission (mb) | 105.16 | 105.19 | −0.03 % | ± 1 % | IAEA IRDFF-II |
| σ̄ Al-27(n,α), U-235 fission (mb) | 0.68689 | 0.6872 | −0.05 % | ± 1 % | IAEA IRDFF-II |
| σ̄ S-32(n,p), U-235 fission (mb) | 66.826 | 66.846 | −0.03 % | ± 1 % | IAEA IRDFF-II |
| fission neutrons above 0.5 MeV (fraction) | 0.8685 | 0.871544 | −0.35 % | ± 2 % | Watt spectrum |
| fission neutron mean energy (MeV) | 2 | 2.03084 | −1.52 % | ± 2.5 % | Watt spectrum |
| Ni-58(n,p) saturation, 1 g (Bq) | 4.2288 × 10⁷ | 4.2152 × 10⁷ | +0.32 % | ± 3 % | IRDFF-II σ̄ + Watt, by hand |
Reactor physics 14
Equilibrium poisoning saturates and is Σf-independent
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| [Xe] saturation ratio 1e13→1e14 | 1.66276 | 1.66276 | < 0.01 % | ± 1 % | φ/(λ_Xe+σ_Xe·φ) |
| Xe-135 reactivity saturates with flux | -1517 pcm at 1e13 → -2523 pcm at 1e14 | pass | — | φ/(λ_Xe+σ_Xe·φ) |
| [I] linear in flux | 10 | 10 | < 0.01 % | ± 1 % | I has no burnup term |
Transients agree with an independent RK4 of the same equations
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| startup 1e14: Xe at 10 h | 7.2284 × 10¹⁴ | 7.2284 × 10¹⁴ | < 0.01 % | ± 0.01 % | RK4 |
| startup 1e14: Xe at 48 h | 1.1488 × 10¹⁵ | 1.1488 × 10¹⁵ | < 0.01 % | ± 0.01 % | RK4 |
| step 100→50 %: Xe at 5 h | 1.7603 × 10¹⁵ | 1.7603 × 10¹⁵ | < 0.01 % | ± 0.01 % | RK4 |
| step 100→50 %: Xe at 30 h | 1.1319 × 10¹⁵ | 1.1319 × 10¹⁵ | < 0.01 % | ± 0.01 % | RK4 |
| iodine pit peak after 1e14 shutdown (h) | 10.15 | 10.147 | +0.03 % | ± 1 % | closed form, D&H §15 |
Inhour periods satisfy the six-group equation
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| inhour ρ = 0.05$ → T 226.9 s | 0.05 | 0.05 | < 0.01 % | ± 0.1 % | inhour eq. |
| inhour ρ = 0.1$ → T 98.5 s | 0.1 | 0.1 | < 0.01 % | ± 0.1 % | inhour eq. |
| inhour ρ = 0.25$ → T 25.4 s | 0.25 | 0.25 | < 0.01 % | ± 0.1 % | inhour eq. |
| inhour ρ = 0.5$ → T 5.7 s | 0.5 | 0.5 | < 0.01 % | ± 0.1 % | inhour eq. |
| inhour ρ = 0.8$ → T 0.9 s | 0.8 | 0.8 | < 0.01 % | ± 0.1 % | inhour eq. |
| small ρ: T·ρ[$] → Σaᵢ/λᵢ (s) | 12.9985 | 13.03 | −0.24 % | ± 1 % | Keepin mean delay |
Mixtures and enrichment 31
4.5 % LEU cascade vs the textbook case
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| SWU per kg product (4.5 % LEU) | 6.87111 | 6.9 | −0.42 % | ± 6 % | value function |
| feed per kg product (4.5 % LEU) | 9.21909 | 9.2 | +0.21 % | ± 6 % | mass balance |
| mass balance F − P − W | -1.7764 × 10⁻¹⁵ | 0 | -1.7764 × 10⁻¹⁵ abs | ± 1e-6 % | conservation |
Elemental fractions vs IUPAC atomic weights
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| H₂O hydrogen (wt%) | 11.1901 | 11.19 | < 0.01 % | ± 1 % | IUPAC masses |
| UO₂ uranium (wt%) | 88.1498 | 88.15 | < 0.01 % | ± 1 % | IUPAC masses |
| H2O wt% sums to 100 | 100 | 100 | < 0.01 % | ± 0.01 % | conservation |
| UO2 wt% sums to 100 | 100 | 100 | < 0.01 % | ± 0.01 % | conservation |
| Ca(OH)2 wt% sums to 100 | 100 | 100 | < 0.01 % | ± 0.01 % | conservation |
Atomic weights and molar masses vs IUPAC/CIAAW 2021
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| atomic weight H | 1.00797 | 1.008 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight B | 10.8135 | 10.81 | +0.03 % | ± 0.1 % | CIAAW 2021 |
| atomic weight C | 12.0106 | 12.011 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight N | 14.0069 | 14.007 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight O | 15.9994 | 15.999 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight Na | 22.9898 | 22.99 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight Al | 26.9815 | 26.982 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight Cl | 35.4521 | 35.45 | +0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight Ca | 40.078 | 40.078 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight Fe | 55.8451 | 55.845 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight Cu | 63.546 | 63.546 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight Zr | 91.2236 | 91.224 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight Cd | 112.414 | 112.41 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight Gd | 157.252 | 157.25 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight W | 183.842 | 183.84 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight Pb | 207.217 | 207.2 | +0.01 % | ± 0.1 % | CIAAW 2021 |
| atomic weight Th | 232.038 | 232.04 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| atomic weight U | 238.029 | 238.03 | < 0.01 % | ± 0.02 % | CIAAW 2021 |
| molar mass UO₂ (g/mol) | 270.028 | 270.03 | < 0.01 % | ± 0.03 % | from CIAAW weights |
| molar mass UF₆ (g/mol) | 352.019 | 352.02 | < 0.01 % | ± 0.03 % | from CIAAW weights |
| molar mass B₄C (g/mol) | 55.2647 | 55.255 | +0.02 % | ± 0.1 % | from CIAAW weights |
| Pu (no stable isotope) = Pu-244 mass | 244.064 | 244.064 | < 0.01 % | ± 0.01 % | AME2020 |
| Ra (no stable isotope) = Ra-226 mass | 226.025 | 226.025 | < 0.01 % | ± 0.01 % | AME2020 |
Counting statistics and units 15
Currie critical level and detection limit
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| Currie L_c (B=100) | 23.2638 | 23.3 | −0.16 % | ± 1 % | Currie 1968 |
| Currie L_d (B=100) | 49.2337 | 49.21 | +0.05 % | ± 1 % | Currie 1968 |
| Currie L_c (B=400) | 46.5276 | 46.6 | −0.16 % | ± 1 % | Currie 1968 |
| Currie L_d (B=400) | 95.7613 | 95.71 | +0.05 % | ± 1 % | Currie 1968 |
| Currie L_c (B=2500) | 116.319 | 116.5 | −0.16 % | ± 1 % | Currie 1968 |
| Currie L_d (B=2500) | 235.344 | 235.21 | +0.06 % | ± 1 % | Currie 1968 |
Units, isomer specific activity, detection decision, optimum tails
| CHECK | APP | REFERENCE | DEVIATION | TOLERANCE | SOURCE |
| 1 Ci in Bq | 3.7000 × 10¹⁰ | 3.7000 × 10¹⁰ | < 0.01 % | ± 1e-9 % | definition |
| 1 R in C/kg | 2.5800 × 10⁻⁴ | 2.5800 × 10⁻⁴ | < 0.01 % | ± 1e-9 % | definition |
| 1 MeV in J | 1.6022 × 10⁻¹³ | 1.6022 × 10⁻¹³ | < 0.01 % | ± 1e-9 % | SI 2019 exact e |
| 1 Gy in rad | 100 | 100 | < 0.01 % | ± 1e-9 % | definition |
| 1 Sv in rem | 100 | 100 | < 0.01 % | ± 1e-9 % | definition |
| 1 y in s (Julian) | 3.1558 × 10⁷ | 3.1558 × 10⁷ | < 0.01 % | ± 1e-9 % | IAEA half_life_sec |
| Tc-99m specific activity (Ci/g) | 5.2744 × 10⁶ | 5.2700 × 10⁶ | +0.08 % | ± 1 % | handbook |
| Currie decision at the boundary, B = 100 | net 24 → detected, net 23 → not; L_c = 23.26 | pass | — | Currie 1968 |
| optimum tails assay (cost ratio 0.5) | 0.00302462 | 0.003025 | −0.01 % | ± 0.1 % | brute-force scan |
Corrections
Errors found by earlier audits, and the release that fixed them. If you used
one of these calculations in an earlier version, recompute it.
- 1.4.1 · HIGH
-
Shielding behind lead, tungsten and iron. Buildup came
from Taylor fits that stopped at 0.5 MeV and borrowed other
materials’ data, and the attenuation counted coherent scattering as
removal. Now: the ANSI/ANS-6.4.3 standard buildup factors for every
material, 15 keV–15 MeV, with the coherent-free attenuation the
standard requires. Dose behind thick lead was low: Cs-137 behind 10 cm
of lead read about half the corrected value, and a third below an
independent slab Monte Carlo that itself leaves out lead
fluorescence; behind 5 cm about 25 % below the corrected value. A
low-energy source immersed in water read up to 2× low.
- 1.4.1 · MEDIUM
-
Fast-neutron activation. Threshold cross sections were
order-of-magnitude estimates, applied to every source as if it emitted
fission neutrons. They are now IAEA IRDFF-II averages over each
source’s own spectrum. Reactor results were 9–43 % low
(O-16(n,p), the N-16 source, most); Fe-54(n,p) with Am-Be was
3.4× low; the D-D generator reported activation for reactions a
2.45 MeV neutron cannot cause.
- 1.4.1 · LOW
-
Activation data consistency. Four product half-lives
and two abundances now match the NUBASE2020 data the tab cites (W-187
was 0.8 % long). The on-screen formula still showed the epithermal
factor 0.45 retired in 1.4.0; the calculation already used 1.
- 1.4.0 · HIGH
-
Dose and shielding, ten parent nuclides. Pb-212, Bi-212,
Ba-140, Np-237, Zr-95, Ce-144, Mo-99, Ra-228, Pb-214 and Ba-131 were
offered without the short-lived progeny that carry most of their gamma
dose. An aged Pb-212 source read about 10× low, and the shield
solver asked for 0.32 cm of lead where 9.95 cm is needed. Each
now has a “+progeny” entry at transient-equilibrium activity.
- 1.4.0 · MEDIUM
-
Reactor period. The one-group stable period was
2.3× too long at +$0.50. It now solves the six-group inhour
equation (Keepin U-235 thermal groups).
- 1.4.0 · MEDIUM
-
Decay Chain tab. The followed branch was credited with
every decay (Po-212 1.56× high). Activities now come from the full
branching solution, with the other branches and any truncation shown.
- 1.4.0 · MEDIUM
-
Neutron activation. The epithermal term used a factor
matching no published convention; Au-197 read 24 % and Mo-98
40 % low. It now follows the Høgdahl convention with
φe per unit lethargy.
- 1.0.5 · HIGH
-
Bateman chains. Members below a short-lived one were
starved: Ra-226 over one year reported Bi-214 about 104×
low. The integrator was replaced with a closed-form solution, checked
above against secular and transient equilibrium.
- 1.0.5 · LOW
-
H*(10) above 1.5 MeV. The conversion from air kerma
fell away where ICRP 74 Table A.21 plateaus, so ambient dose
equivalent for high-energy photons read low. All 25 rows now match the
printed table.
Known limitations
Stated because a validation page that lists only strengths is marketing.
- Point sources only, single-layer shields, gamma only — no neutron dose.
- Buildup factors are the ANSI/ANS-6.4.3 infinite-medium values applied to
a slab, which overstates the dose behind a wall — per the slab Monte
Carlo above, 1.1–1.2× behind lead and 1.4–1.7× behind
concrete and water, 1 m back. Per-line transmission is capped at 1.
- Air is optional and off by default (vacuum, as published dose constants
assume). Switched on, it is an infinite-air kernel: no ground or room
scatter.
- Neutron cross sections cover 298 of 3,383 nuclides (8.8 %). A
missing value is shown as missing, never as zero.
- Fast-neutron cross sections are IAEA IRDFF-II averages over the chosen
source’s spectrum. For Am-Be, three reactions have no value: the
published spectrum is too coarse above 10 MeV for them.
- Activation neglects target burn-up and self-shielding.
- Reactor period uses Keepin’s U-235 thermal delayed-neutron
groups; Pu-239 and fast-spectrum cores differ. Xe-135 is a one-group,
spatially uniform model.
- Evaluated data is shown as published: 91 ground states and 11 isomers
have branches that NUBASE2020 sums past 100.5 %, and they are not
renormalised.
- No uncertainty propagation. Evaluated values are used as point estimates.
Found a number that disagrees with your reference? Email
[email protected]
with the inputs and units you used, the value the app showed, and the value
you expected with its source. Accuracy reports are looked at first, and a
confirmed one is added to this page.