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Radioactive Decay Calculator

Model radioactive decay over time with the exponential decay formula. Generate a decay curve showing how a radioactive sample diminishes over multiple half-lives.

Radioactive decay is the fundamental probabilistic process of nuclear physics: an unstable nucleus has a fixed probability per unit time of decaying, regardless of how old it is or what surrounds it. That probability is captured by the decay constant λ, and from λ comes the half-life t₁/₂ = ln(2)/λ — the time for half a sample to decay. Because decay is exponential, after one half-life 50% remains, after two 25%, after three 12.5%, after ten about 0.1%, and after twenty essentially none — but never zero exactly.

This calculator handles the standard problem: given an initial amount, a half-life, and an elapsed time, find what remains. It complements the related "half-life" calculator (which can also solve for half-life given amounts, or solve for elapsed time given amounts). Use this one when you have a known isotope and need to know what fraction is left at a future time — radioactive waste planning, medical isotope inventory, or carbon-14 dating predictions.

The decay law works for any radioactive isotope: short half-life (technetium-99m at 6 hours for medical imaging), long half-life (uranium-238 at 4.5 billion years for geological dating), and everything in between. It's also temperature-, pressure-, and chemistry-independent — uranium decays at exactly the same rate in a hot lava flow as in a cold mountain stream. The few exceptions (rare electron-capture decays influenced by electronic environment) are research curiosities, not practical concerns.

Inputs

Results

Remaining

250.00

% Remaining

25.00%

Half-Lives

2.00

Decay Curve

Radioactive Decay Results

ParameterValue
Initial Amount (N0)1,000
Half-Life5,730 years
Time Elapsed11,460 years
Half-Lives Elapsed2.0000
Remaining Amount250.0000
Decayed Amount750.0000
Percent Remaining25.0000%
Decay Constant (lambda)1.209681e-4 / years
Activity (lambda x N)3.0242e-2 / years
Mean Lifetime (1/lambda)8266.6426 years
Last updated:

Formula

**Exponential decay law:** N(t) = N₀ × (1/2)^(t / t₁/₂) Or equivalently: N(t) = N₀ × e^(−λt) Where: - **N(t)**: amount remaining at time t - **N₀**: initial amount - **t**: elapsed time - **t₁/₂**: half-life (same time units as t) - **λ**: decay constant = ln(2) / t₁/₂ ≈ 0.693 / t₁/₂ **Activity (rate of decay):** A(t) = λ × N(t) = A₀ × (1/2)^(t/t₁/₂) Units: becquerel (Bq) = decays per second; or curie (Ci) = 3.7 × 10¹⁰ Bq. **Fraction remaining at multiples of half-life:** | Half-lives elapsed | Fraction remaining | |---|---| | 1 | 50% | | 2 | 25% | | 3 | 12.5% | | 4 | 6.25% | | 5 | 3.13% | | 6 | 1.56% | | 7 | 0.78% | | 10 | 0.098% | | 20 | 0.0001% (1 ppm) | **Worked example: Tc-99m (medical imaging)** t₁/₂ = 6.0 hours. Hospital receives 5 GBq at 8 AM. At noon (4 hr later): N(4)/N₀ = (1/2)^(4/6) = 2^(−0.667) = 0.630 N(4) = 5 × 0.630 = **3.15 GBq** remaining at noon By 8 PM (12 hr = 2 half-lives): N = 5 × 0.25 = 1.25 GBq. **Worked example: carbon-14 in a fossil** A bone has 30% of the C-14 of a living organism. How old? t/t₁/₂ = log₂(N₀/N) = log(1/0.30)/log(2) = 1.737 t = 1.737 × 5730 yr = **9950 years** old (estimate) **Common decay modes:** | Decay type | Particle emitted | Effect on Z, A | |---|---|---| | α (alpha) | He-4 nucleus | Z−2, A−4 | | β⁻ (beta minus) | electron + antineutrino | Z+1, A unchanged | | β⁺ (beta plus / positron) | positron + neutrino | Z−1, A unchanged | | EC (electron capture) | neutrino (captures e⁻) | Z−1, A unchanged | | γ (gamma) | photon | no change in Z, A | | n (neutron emission) | neutron | A−1 | | Spontaneous fission | two large fragments | massive change | **Activity comparison (orders of magnitude):** | Source | Approximate activity | |---|---| | 1 µg I-131 (medical scan) | 4.6 × 10⁹ Bq | | Annual radon exposure (US avg) | 2 × 10⁻¹⁰ Bq/L air | | Banana (K-40) | ~15 Bq | | Coffee cup of seawater | ~13 Bq | | Human body (mostly K-40, C-14) | ~7000 Bq | | 1 gram of Cs-137 | 3.2 TBq | | Chernobyl reactor 4 core, total release | ~12,000 PBq |

How to use this calculator

  1. Pick the isotope of interest and look up its half-life (carbon-14: 5730 yr; iodine-131: 8.02 days; Tc-99m: 6.0 hr).
  2. Enter the initial amount (atoms, mass, or activity — units carry through).
  3. Enter elapsed time in the same units as the half-life (yr/yr, hr/hr, s/s).
  4. Pick the time unit; the calculator handles unit conversion within the same dimension.
  5. Output: amount remaining and activity (if applicable).
  6. For "how much before safe to handle?" problems, define a target N or activity and back-solve for t.

Worked examples

Tc-99m scan kit decay during the day

**Scenario:** Nuclear medicine ordered 10 GBq Tc-99m at 8 AM for a 2 PM patient scan. How much remains at scan time? **Calculation:** Tc-99m half-life = 6.0 hr. Elapsed = 6 hr = 1 half-life. N = 10 × 0.5 = 5 GBq. **Result:** 5 GBq at scan time — half the morning dose. Nuclear medicine departments time orders precisely because tracers are unusable within a few half-lives. By next day (24 hr, 4 half-lives), only 0.625 GBq remains — insufficient for most scans.

Carbon-14 fossil dating

**Scenario:** Wooden artifact has 8% of the C-14 of a living tree. Date it. **Calculation:** Fraction remaining = 0.08. Half-lives elapsed = log(1/0.08)/log(2) = 1.10/0.301 = 3.64. Time = 3.64 × 5730 = 20,855 years old. **Result:** Approximately 21,000 years old — Last Glacial Maximum era (Pleistocene), possibly Solutrean culture site. C-14 dating is reliable to about 50,000 years; beyond that, the remaining C-14 is too low to measure accurately.

Iodine-131 thyroid treatment recovery

**Scenario:** Patient receives I-131 thyroid ablation dose of 1.5 GBq. When will residual activity drop below 30 MBq (release threshold)? **Calculation:** Need N/N₀ = 0.03/1.5 = 0.02. Half-lives = log(1/0.02)/log(2) = 5.64. I-131 half-life = 8.02 days. Time = 5.64 × 8.02 = 45.2 days. **Result:** ~45 days for the patient's residual activity to drop below 30 MBq. Hospitals typically discharge thyroid I-131 patients with restrictions for 2–3 weeks (limited contact with children, pregnant women). After 6 weeks, almost no activity remains. The biological half-life is shorter than physical half-life because urinary excretion accelerates clearance.

When to use this calculator

**Use radioactive decay calculations for:**

- **Medical isotope timing**: ordering, scan planning, patient release after treatment. - **Radioactive waste planning**: how long until disposal containers reach safe activity? - **Carbon-14 dating**: archaeological and geological age estimation (organic samples, < 50k years old). - **Uranium/thorium series dating**: older samples using U-238 (4.5 billion yr), K-40 (1.25 billion yr), etc. - **Radiation safety planning**: facility design, exposure modeling, evacuation timelines. - **Smoke detectors**: Am-241 source longevity (~450 yr half-life, essentially constant over device lifetime). - **Nuclear reactor operations**: fuel decay heat after shutdown, fission product timelines. - **Geochemistry**: K-Ar dating of volcanic rocks, lead isotope ratios for ore body genesis.

**Important isotopes by use case:**

**Medical imaging:**

- Tc-99m: 6 hr (most common, ~85% of nuclear medicine scans) - F-18: 110 min (PET scans with FDG) - I-131: 8.02 days (thyroid imaging and therapy) - Tl-201: 73 hr (cardiac perfusion)

**Industrial / safety:**

- Am-241: 432 yr (smoke detectors, industrial gauges) - Co-60: 5.27 yr (sterilization, radiotherapy) - Cs-137: 30.2 yr (sterilization, industrial gauging) - Sr-90: 28.8 yr (legacy fallout, betavoltaic batteries)

**Geological dating:**

- C-14: 5730 yr (organic, < 50k yr) - K-40 → Ar-40: 1.25 billion yr (volcanic rocks) - U-235 → Pb-207: 704 million yr (zircon, oldest rocks) - U-238 → Pb-206: 4.47 billion yr (oldest Earth materials) - Rb-87 → Sr-87: 49 billion yr (early Earth, lunar samples)

**Safety thresholds:**

- After 5 half-lives: ~3% remains, often considered "practically clear." - After 10 half-lives: ~0.1% remains — usually negligible. - After 20 half-lives: ~1 ppm — essentially gone.

**Branching decays:**

Some isotopes have multiple decay modes (e.g., K-40 decays by both β⁻ to Ca-40 AND electron capture to Ar-40). The total decay constant is the sum of branch constants: λ_total = λ_β + λ_EC. Half-life uses the total.

**Useful for environmental and forensic work:**

- **Cs-137 fallout dating**: Cs-137 from atmospheric weapons testing peaked 1955-1965. Soil or lake sediment cores show distinct Cs-137 signals that can date layers within ±1 year. - **Pu-239 in legacy contamination**: 24,110 yr half-life means weapons-era contamination persists effectively forever. - **Sr-90 in milk and bones**: shorter half-life means measurable in tissues; useful for monitoring environmental fallout history.

Common mistakes to avoid

  • Treating decay as linear. After 2 half-lives, 25% remains (not 0%, not 50% — exponential).
  • Mismatched time units. If half-life is in years and elapsed time is in days, you get nonsense.
  • Confusing the "10 half-lives" guideline (~0.1% remaining) with "10 mean lifetimes" (which is much longer — mean lifetime τ = 1/λ = t₁/₂/ln(2) ≈ 1.44 × t₁/₂).
  • Forgetting biological half-life. Drugs and isotopes are cleared by urinary excretion and metabolism, often faster than physical decay alone would predict.
  • Using physical half-life for whole-body dose. Effective half-life = (physical × biological) / (physical + biological).
  • Ignoring decay chain daughters. Many radioactive isotopes decay into other radioactive isotopes; total radioactivity may be higher than just the parent.
  • Trying to extrapolate to far future. After 10+ half-lives the math is correct but practically irrelevant — uncertainty in initial amount and counting statistics dominates.

Frequently Asked Questions

Sources & further reading

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