Formula: Nt = N0 × (1/2)t/t½
Time in the same units as half-life
Time units (years, days, seconds, etc.)
Time in the same units as half-life
Time units (years, days, seconds, etc.)
Half-life is the time required for exactly half of a given quantity of a radioactive substance to undergo decay. This fundamental concept in nuclear physics describes how unstable atomic nuclei lose energy by emitting radiation over time. The half-life remains constant for any given isotope regardless of how much of the substance is present or environmental conditions like temperature or pressure, making it one of the most reliable measures in science.
The term "half-life" was coined by Ernest Rutherford in 1907, though the phenomenon of radioactive decay was discovered by Henri Becquerel in 1896. Understanding half-life is crucial for numerous applications ranging from carbon dating in archaeology to medical imaging and cancer treatment in healthcare, from nuclear power generation to environmental monitoring of radioactive contamination. The predictable nature of radioactive decay allows scientists to use it as a precise "clock" for measuring time scales from milliseconds to billions of years.
Radioactive decay follows an exponential function, meaning the rate of decay is proportional to the amount of substance remaining. This creates a characteristic decay curve that never quite reaches zero but approaches it asymptotically. The fundamental equation governing radioactive decay can be expressed in several equivalent forms, each useful for different types of calculations.
Three Equivalent Decay Formulas:
1. Using Half-Life (t½):
N(t) = N0 × (1/2)t/t½
Most intuitive form - shows how many half-lives have elapsed
2. Using Decay Constant (λ):
N(t) = N0 × e-λt
Standard exponential decay form used in physics
3. Using Mean Lifetime (τ):
N(t) = N0 × e-t/τ
Alternative form emphasizing average particle lifetime
Where:
These three formulas are mathematically equivalent because of the relationships between the constants: λ = ln(2)/t½and τ = 1/λ = t½/ln(2). The half-life form is most intuitive for practical calculations, while the decay constant form is preferred in theoretical physics because it directly relates to the fundamental probability of decay events.
While half-life is the most commonly used measure, physicists use three related constants to characterize radioactive decay. Each provides a different perspective on the same underlying decay process, and knowing any one allows you to calculate the others using simple mathematical relationships.
The time required for half the atoms to decay. Most intuitive measure, easy to visualize.
Example:
Carbon-14: t½ = 5,730 years
After 5,730 years, 100g → 50g
After 11,460 years, 100g → 25g
After 17,190 years, 100g → 12.5g
Average time an atom exists before decaying. Related to half-life by factor of ln(2).
Formula:
τ = t½ / ln(2)
τ ≈ 1.443 × t½
For C-14:
τ = 5,730 / 0.693
τ ≈ 8,267 years
Probability of decay per unit time. Used in theoretical physics and rate equations.
Formula:
λ = ln(2) / t½
λ ≈ 0.693 / t½
For C-14:
λ = 0.693 / 5,730
λ ≈ 1.21 × 10-4 yr-1
Conversion Between Constants:
t½ = τ × ln(2)
t½ = ln(2) / λ
τ = 1 / λ
These relationships allow converting between any decay constant representation. Our calculator's Constant Conversion tab automatically performs these conversions.
One of the most famous applications of half-life is radiocarbon dating, developed by Willard Libby in 1949 (for which he won the Nobel Prize in Chemistry in 1960). This technique revolutionized archaeology, geology, and other fields by providing a reliable method to determine the age of organic materials up to about 50,000 years old.
How Carbon-14 Dating Works:
Step 1: Formation in Atmosphere
Cosmic rays from space collide with nitrogen-14 atoms in the upper atmosphere, converting them to carbon-14. This process continuously produces radioactive carbon at a relatively constant rate.
Step 2: Incorporation into Living Organisms
Plants absorb carbon-14 through photosynthesis along with stable carbon-12. Animals consume plants, incorporating the same ratio of C-14 to C-12 as the atmosphere. Living organisms maintain this equilibrium ratio while alive.
Step 3: Decay After Death
When an organism dies, it stops exchanging carbon with the environment. The C-14 begins to decay to nitrogen-14 with a half-life of 5,730 years, while stable C-12 remains constant. The ratio of C-14 to C-12 decreases predictably.
Step 4: Measuring Age
By measuring the remaining C-14 in a sample and comparing it to the expected amount in a living organism, scientists can calculate how long ago the organism died using the half-life formula.
Example Calculation: Dating a Fossil
Problem:
An archaeologist finds a wooden artifact that contains 25% of the C-14 found in living trees. How old is the artifact?
Given Information:
Solution:
0.25 = 1.00 × (1/2)t/5730
0.25 = (1/2)t/5730
Taking logarithm of both sides:
ln(0.25) = (t/5730) × ln(0.5)
-1.386 = (t/5730) × (-0.693)
t = (-1.386 × 5730) / (-0.693)
t ≈ 11,460 years
Interpretation:
The artifact is approximately 11,460 years old, which is exactly 2 half-lives (5,730 × 2). This makes sense: after one half-life (5,730 years), 50% remains; after two half-lives, 25% remains. The artifact dates to approximately 9,460 BCE, during the early Neolithic period.
Half-life calculations extend far beyond archaeological dating, playing crucial roles in medicine, energy production, environmental science, and fundamental physics research. Understanding radioactive decay is essential for safely harnessing nuclear energy and managing radioactive materials.
Radioactive isotopes with specific half-lives are used in diagnostic imaging and cancer therapy. Short half-lives minimize radiation exposure while providing clear images or targeted treatment.
Technetium-99m: t½ = 6 hours
Used in SPECT scans for heart, bone, and organ imaging
Fluorine-18: t½ = 110 minutes
Used in PET scans for cancer detection
Iodine-131: t½ = 8 days
Treats thyroid cancer and hyperthyroidism
Understanding half-lives is crucial for nuclear reactor operation and spent fuel management. Uranium and plutonium isotopes with different half-lives require specific handling procedures.
Uranium-235: t½ = 704 million years
Primary nuclear fuel, long-term stability
Plutonium-239: t½ = 24,110 years
Produced in reactors, requires long-term storage
Iodine-131: t½ = 8 days
Fission product, concern in accidents
Different isotopes with varying half-lives allow dating of materials from thousands to billions of years old, enabling scientists to determine Earth's age and geological history.
Potassium-40: t½ = 1.25 billion years
Dating ancient rocks and minerals
Uranium-238: t½ = 4.47 billion years
Dating oldest Earth rocks, meteorites
Rubidium-87: t½ = 48.8 billion years
Dating very ancient geological formations
Half-life determines how long radioactive materials remain hazardous, guiding safety protocols, storage requirements, and decontamination efforts after nuclear incidents.
Safety Rule: After 10 half-lives, activity drops to ~0.1%
Material considered relatively safe
Example - Cesium-137: t½ = 30 years
Chernobyl exclusion zone: 300 years (10 half-lives) before safe levels
Currently at ~40 years since 1986 accident (≈1.3 half-lives)
The mathematical elegance of half-life lies in its simplicity and predictability. Unlike many natural processes, radioactive decay follows a perfect exponential curve that is completely independent of external conditions. This makes it an ideal tool for precise measurements and predictions.
Key Mathematical Properties:
1. Constant Half-Life
The half-life is constant regardless of initial amount. Whether you start with 1 gram or 1,000 kilograms, half decays in the same time period. This property is unique to exponential processes.
2. Never Reaches Zero
Mathematically, the amount approaches but never reaches zero. In practice, quantum mechanics ensures that the last atom eventually decays, but the exponential model remains valid for macroscopic quantities.
3. Predictable Fractions
After n half-lives, exactly (1/2)n remains: 1 half-life = 50%, 2 half-lives = 25%, 3 half-lives = 12.5%, 4 half-lives = 6.25%, and so on. This makes quick mental calculations possible.
4. Independent of Temperature & Pressure
Unlike chemical reactions, radioactive decay is unaffected by temperature, pressure, chemical bonding, or any external conditions. The decay occurs in the nucleus, isolated from environmental influences.
Quick Reference: Decay After N Half-Lives
1 t½
50.0%
2 t½
25.0%
3 t½
12.5%
4 t½
6.25%
5 t½
3.125%
6 t½
1.563%
7 t½
0.781%
10 t½
0.098%
Ensure time elapsed and half-life use the same units (both in years, days, hours, etc.). Mismatched units are the most common source of calculation errors. Convert before calculating.
Quick check: Divide elapsed time by half-life to get number of half-lives. If you get 3, expect about 12.5% remaining. This validates your detailed calculation.
After 10 half-lives, less than 0.1% remains—essentially negligible. This guides waste storage timelines and safety protocols for radioactive materials.
In carbon dating, work with ratios (Nt/N0) rather than absolute amounts. This eliminates the need to know exact initial quantities.
When solving for time or half-life, logarithms are essential. Remember: ln(0.5) = -0.693 and ln(2) = 0.693. These constants appear frequently in decay calculations.
Real measurements have uncertainty. Carbon-14 dates are typically given as ± 30-50 years. Report results with appropriate precision reflecting measurement accuracy.
Half-life represents one of nature's most reliable clocks, providing scientists with a precise tool for measuring time scales from microseconds to billions of years. From dating ancient artifacts to treating cancer patients, from powering cities to exploring the cosmos, radioactive decay and half-life calculations underpin countless modern technologies and scientific discoveries.
Our half-life calculator simplifies these complex calculations, handling the exponential mathematics automatically while showing you the underlying principles. Whether you're a student learning about radioactive decay, a researcher conducting carbon dating analysis, or simply curious about nuclear physics, understanding half-life deepens your appreciation for the atomic world and the mathematical beauty of exponential processes.
The elegance of half-life lies in its simplicity—a single number characterizing the decay rate of each isotope, unchanging regardless of conditions or quantity. This constancy makes radioactive decay one of the most reliable phenomena in nature, a fundamental property of matter that allows us to peer into the past, diagnose diseases, generate clean energy, and understand the very building blocks of our universe. Whether calculating the age of a 50,000-year-old fossil or determining how long radioactive waste must be safely stored, half-life calculations provide the mathematical foundation for working safely and effectively with radioactive materials.