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How Radioactive Half-Life Works

CalculatorGlobe Team February 23, 2026 13 min read Math

Radioactive half-life is one of the most important concepts in nuclear physics, with applications ranging from dating ancient artifacts to treating cancer. At its core, half-life describes the predictable rate at which unstable atoms transform into different elements, following the elegant mathematics of exponential decay. Understanding this concept connects abstract mathematics to tangible real-world science.

This guide explains the half-life concept from first principles, derives the key formulas, works through detailed calculation examples, and explores the fascinating applications that make half-life relevant to archaeology, medicine, energy production, and environmental science.

What Is Radioactive Half-Life?

Radioactive half-life is the time required for exactly half of the atoms in a radioactive sample to undergo decay. If you start with 1,000 unstable atoms, after one half-life you will have approximately 500. After two half-lives, approximately 250 remain. After three half-lives, approximately 125. This pattern continues indefinitely, with the quantity halving during each successive time interval.

The key insight is that half-life is a property of the isotope itself, not of the sample size. Whether you have a gram or a kilogram of a radioactive substance, the half-life remains the same. The decay of any individual atom is random and unpredictable, but the statistical behavior of large numbers of atoms is remarkably consistent and follows a precise mathematical curve.

Successive Half-Lives: Starting with 1,000 Atoms

Start: 1,000 atoms (100%)

After 1 half-life: 500 atoms (50%)

After 2 half-lives: 250 atoms (25%)

After 3 half-lives: 125 atoms (12.5%)

After 4 half-lives: 62.5 atoms (6.25%)

After 5 half-lives: 31.25 atoms (3.125%)

After 10 half-lives: 0.98 atoms (0.098%)

Notice that the sample never truly reaches zero. Each half-life removes half of what remains, so there is always a smaller and smaller residual. In practice, after about 10 half-lives, less than 0.1% of the original material remains, and the radioactivity becomes negligible for most purposes.

The Exponential Decay Formula

The mathematical description of radioactive decay uses an exponential function. There are two equivalent forms of the decay equation:

Exponential Decay Formulas

N(t) = N0 x (1/2)^(t / t_half)

N(t) = N0 x e^(-lambda x t)

N(t) = quantity remaining at time t

N0 = initial quantity

t_half = half-life

lambda (λ) = decay constant

e = Euler's number (approximately 2.71828)

The first form is intuitive: you raise one-half to the power of how many half-lives have elapsed. The second form uses the natural exponential function and the decay constant, which is more convenient for calculus-based derivations and more general mathematical analysis.

Calculating the Decay Constant

The decay constant (λ) and the half-life are inversely related through the natural logarithm of 2:

Decay Constant Formula

λ = ln(2) / t_half = 0.693 / t_half

Conversely: t_half = ln(2) / λ = 0.693 / λ

The decay constant represents the probability per unit time that any given atom will decay. A larger decay constant means a shorter half-life and faster decay. For example, iodine-131 has a decay constant of 0.0866 per day (half-life of 8 days), while carbon-14 has a decay constant of 1.21 x 10^-4 per year (half-life of 5,730 years).

Another useful quantity is the mean lifetime (τ), which equals 1/λ. The mean lifetime is the average time a single atom will survive before decaying, and it equals the half-life divided by 0.693, making it about 44% longer than the half-life.

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Step-by-Step Calculation Examples

Example 1: Remaining Quantity After a Given Time

A laboratory has 80 grams of iodine-131, which has a half-life of 8.02 days. How much remains after 24 days?

Step 1: Calculate the number of half-lives elapsed.

Number of half-lives = t / t_half = 24 / 8.02 = 2.994

Step 2: Apply the decay formula.

N(t) = 80 x (1/2)^2.994 = 80 x 0.1255 = 10.04 grams

After 24 days, approximately 10.04 grams of iodine-131 remain out of the original 80 grams.

Example 2: Finding Elapsed Time

A sample of strontium-90 (half-life = 28.8 years) originally contained 200 mg. If only 25 mg remains, how much time has passed?

Step 1: Set up the equation.

25 = 200 x (1/2)^(t / 28.8)

Step 2: Divide both sides by 200.

0.125 = (1/2)^(t / 28.8)

Step 3: Take the logarithm of both sides.

ln(0.125) = (t / 28.8) x ln(0.5)

-2.079 = (t / 28.8) x (-0.693)

Step 4: Solve for t.

t / 28.8 = 2.079 / 0.693 = 3.0

t = 3.0 x 28.8 = 86.4 years

Verification: 25 mg is 1/8 of 200 mg, and (1/2)^3 = 1/8, confirming exactly 3 half-lives have passed.

Example 3: Determining Half-Life from Data

A researcher measures an unknown isotope and finds that a 500-gram sample decays to 312.5 grams in 45 minutes. What is the half-life?

Step 1: Set up the equation.

312.5 = 500 x (1/2)^(45 / t_half)

Step 2: Simplify.

0.625 = (1/2)^(45 / t_half)

Step 3: Take the natural log of both sides.

ln(0.625) = (45 / t_half) x ln(0.5)

-0.4700 = (45 / t_half) x (-0.6931)

Step 4: Solve for t_half.

45 / t_half = 0.4700 / 0.6931 = 0.6781

t_half = 45 / 0.6781 = 66.4 minutes

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Half-Lives of Common Isotopes

Radioactive half-lives span an extraordinary range, from fractions of a second to billions of years. Here are some of the most commonly encountered isotopes and their half-lives:

Isotope Half-Life Decay Type Primary Use
Polonium-214164 microsecondsAlphaNuclear research
Fluorine-18110 minutesBeta-plusPET scans
Technetium-99m6.01 hoursGammaMedical imaging
Iodine-1318.02 daysBeta-minusThyroid treatment
Phosphorus-3214.3 daysBeta-minusBiology research
Cobalt-605.27 yearsBeta-minusRadiation therapy
Strontium-9028.8 yearsBeta-minusRTGs, fallout studies
Cesium-13730.2 yearsBeta-minusIndustrial gauging
Carbon-145,730 yearsBeta-minusArchaeological dating
Plutonium-23924,100 yearsAlphaNuclear fuel
Uranium-235704 million yearsAlphaNuclear fuel, dating
Uranium-2384.47 billion yearsAlphaGeological dating

Applications of Half-Life

The concept of half-life extends far beyond physics textbooks. It has practical applications in fields ranging from archaeology to oncology.

Carbon-14 Dating Explained

Carbon-14 dating (radiocarbon dating) is the most famous application of half-life. Living organisms continuously absorb carbon from the environment, including a small fraction of radioactive carbon-14 along with stable carbon-12. When an organism dies, it stops absorbing new carbon, and the carbon-14 begins to decay with a half-life of 5,730 years while the carbon-12 remains stable.

By measuring the ratio of carbon-14 to carbon-12 in an archaeological sample and comparing it to the ratio in living organisms, scientists can calculate how long ago the organism died. For example, if a wooden artifact has half the carbon-14 content of a living tree, it is approximately 5,730 years old (one half-life). If it has one-quarter the content, it is approximately 11,460 years old (two half-lives).

Carbon-14 Dating Example

An archaeological team finds wooden beams in an ancient settlement. Analysis shows the carbon-14 activity is 37% of the activity in living wood.

Given: N(t)/N0 = 0.37, t_half = 5,730 years

Formula: 0.37 = (1/2)^(t / 5,730)

ln(0.37) = (t / 5,730) x ln(0.5)

-0.9943 = (t / 5,730) x (-0.6931)

t / 5,730 = 1.4346

t = 8,220 years

The wooden beams are approximately 8,220 years old, placing the settlement in the early Neolithic period.

Medical Applications

Nuclear medicine relies heavily on half-life to balance diagnostic or therapeutic effectiveness against radiation exposure. Technetium-99m, with its 6-hour half-life, is used in over 40 million medical imaging procedures worldwide each year. Its short half-life means patients receive useful diagnostic images while the radioactivity diminishes quickly after the procedure.

Iodine-131 treats hyperthyroidism and thyroid cancer because iodine naturally concentrates in the thyroid gland. Its 8-day half-life provides sustained radiation delivery to the targeted tissue. Fluorine-18, with a 110-minute half-life, is the tracer used in PET (positron emission tomography) scans that detect cancer, heart disease, and neurological conditions.

Nuclear Energy and Waste

Nuclear waste management is fundamentally a half-life problem. Spent nuclear fuel contains isotopes with vastly different half-lives. Short-lived fission products like cesium-137 (30.2 years) and strontium-90 (28.8 years) dominate the radioactivity for the first few centuries but decay to negligible levels within about 300 years (approximately 10 half-lives). Long-lived actinides like plutonium-239 (24,100 years) remain hazardous for hundreds of thousands of years, which is why nuclear waste storage facilities must be designed for geological timescales.

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Tips for Solving Half-Life Problems

  • Identify what you are solving for. Half-life problems always involve four quantities: initial amount, remaining amount, elapsed time, and half-life. You will be given three and asked to find the fourth. Identifying the unknown first helps you choose the correct rearrangement of the formula.
  • Check if the problem involves whole half-lives. When the elapsed time is an exact multiple of the half-life, you can solve by repeatedly halving. Three half-lives means the sample is at 1/8 of its original amount. This avoids logarithms entirely.
  • Keep units consistent. If the half-life is given in years and the elapsed time in days, convert before calculating. Mixing units is the single most common error in half-life problems.
  • Use logarithms for non-integer half-lives. When the elapsed time does not divide evenly into the half-life, you must use the logarithmic form of the equation. Practice taking natural logarithms on your calculator.
  • Verify your answer makes physical sense. The remaining quantity must be less than the initial quantity. The elapsed time must be positive. If your answer violates either condition, recheck your algebra.
  • Remember the 10-half-life rule of thumb. After 10 half-lives, less than 0.1% of the original material remains. This provides a quick sanity check for your calculations.

Common Mistakes to Avoid

  • Subtracting half the amount for each half-life instead of halving the remaining amount. If you start with 100 grams, after one half-life you have 50 grams. After two half-lives, you have 25 grams (half of 50), not 0 grams (100 minus 50 minus 50). Each half-life removes half of what is currently present, not half of the original amount.
  • Confusing half-life with mean lifetime. The mean lifetime is about 1.44 times the half-life. Using one in place of the other will give you an incorrect answer. Always check whether the problem gives you half-life or mean lifetime.
  • Applying the formula to non-radioactive processes. While exponential decay appears in pharmacology, economics, and other fields, the decay constants are different from radioactive half-lives. Make sure you are using the appropriate constant for the process you are modeling.
  • Rounding intermediate calculations. Logarithmic calculations lose precision quickly when you round intermediate steps. Carry at least four significant figures through your calculations and only round the final answer.
  • Assuming linear decay. Radioactive decay is exponential, not linear. The amount lost per unit time decreases as the sample shrinks. A graph of remaining quantity versus time is a curve, not a straight line.

Frequently Asked Questions

Under normal conditions, radioactive decay cannot be altered by changes in temperature, pressure, chemical state, or electromagnetic fields. The decay rate is governed by the nuclear forces within the atom, which are unaffected by external conditions. Extremely rare exceptions exist in certain electron capture decay modes where extreme physical conditions (such as those in stellar interiors) can slightly alter decay rates, but these effects are negligible under any conditions achievable on Earth.

The half-life of an isotope depends on the stability of its nuclear configuration, which is determined by the balance between the strong nuclear force (which holds protons and neutrons together) and the electromagnetic repulsion between protons. Isotopes with a less stable nuclear arrangement have shorter half-lives because they are more likely to undergo a decay event at any given moment. The specific quantum mechanical properties of each nucleus determine its unique decay probability.

When a radioactive atom decays, it transforms into a different element or isotope called a daughter product. The type of transformation depends on the decay mode: alpha decay reduces the atomic number by 2, beta-minus decay increases it by 1, and beta-plus decay decreases it by 1. The daughter product may itself be radioactive and undergo further decay, creating a decay chain that continues until a stable isotope is reached. For example, uranium-238 decays through a chain of 14 steps before reaching stable lead-206.

Carbon-14 dating is reliable for organic materials up to approximately 50,000 years old, which represents about 8-9 half-lives of carbon-14. Beyond this age, so little carbon-14 remains that measurements become unreliable. For samples younger than 50,000 years, the technique has an accuracy of roughly plus or minus 40 to 80 years for well-preserved specimens. Calibration curves derived from tree ring data improve accuracy by accounting for historical variations in atmospheric carbon-14 concentration.

Half-life is the time required for half of a radioactive sample to decay. Mean lifetime (also called average lifetime) is the average time an individual atom survives before decaying. Mathematically, mean lifetime equals the half-life divided by the natural logarithm of 2 (approximately 0.693). This means the mean lifetime is always about 44% longer than the half-life. Both quantities describe the same decay process but from different statistical perspectives.

The exponential decay formula is a statistical model that works best for large numbers of atoms. With billions or trillions of atoms (which is typical for any measurable quantity of material), the formula is extremely accurate. For very small numbers of atoms, individual decay events become noticeable as random fluctuations, and the smooth exponential curve becomes a staircase of discrete events. In practice, even a microgram of radioactive material contains enough atoms for the statistical model to apply.

In nuclear medicine, half-life determines how long a radioactive tracer remains active in the body. Technetium-99m, with a 6-hour half-life, is the most widely used medical isotope because it provides clear imaging results while decaying quickly enough to limit radiation exposure. Iodine-131, with an 8-day half-life, is used to treat thyroid conditions because it remains active long enough to deliver therapeutic radiation to the thyroid gland. The half-life must balance imaging or treatment effectiveness against patient safety.

Sources & References

  1. Nuclear Regulatory Commission — Definition and fundamentals of radioactive half-life: nrc.gov
  2. U.S. Environmental Protection Agency — Radioactive decay processes and health effects: epa.gov
  3. HyperPhysics - Georgia State University — Radioactive half-life and decay calculations: hyperphysics.phy-astr.gsu.edu
  4. Nuclear Regulatory Commission — Radiation basics and nuclear science fundamentals: nrc.gov
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Last updated: February 23, 2026