Half Life Calculator

Physics Class 12 - Nuclear Physics

Remaining

25.00

Decayed

75.00

Formula

N = N₀ × (½)^(t/t½)

Understanding Half-Life: Nuclear Physics Class 12 Complete Guide

Half-life is one of the most fascinating and important concepts in Nuclear Physics, covered in Class 12 Physics Chapter 13. This fundamental property of radioactive substances determines how quickly atoms decay and has profound implications in medicine, archaeology, energy production, and our understanding of the universe itself. Understanding half-life allows scientists to date ancient artifacts, doctors to administer safe radiation treatments, and engineers to manage nuclear waste safely.

What is Half-Life?

The half-life (t1/2) of a radioactive substance is defined as the time required for half of the radioactive nuclei in a sample to undergo radioactive decay. This is a statistical property that applies to large numbers of atoms. For any single atom, decay is completely random and unpredictable - we cannot say when a particular atom will decay. However, for billions of atoms, the statistical behavior is remarkably consistent and predictable.

After one half-life, exactly 50% of the original atoms remain undecayed. After two half-lives, 25% remain (half of the 50%). After three half-lives, 12.5% remain, and this pattern continues geometrically. This exponential decay pattern is fundamental to all radioactive processes.

The Decay Formula

N = N₀ × (½)^(t/t1/2)
N = N₀ × e^(-λt) where λ = 0.693/t1/2

Where:

  • N₀ = Initial number of atoms (at t = 0)
  • N = Number of atoms remaining after time t
  • t1/2 = Half-life of the radioactive substance
  • t = Time elapsed
  • λ = Decay constant (probability of decay per unit time)

The Exponential Decay Pattern

TimeFraction RemainingPercentageDecayed
0 (start)1100%0%
1 half-life1/250%50%
2 half-lives1/425%75%
3 half-lives1/812.5%87.5%
4 half-lives1/166.25%93.75%
5 half-lives1/323.125%96.875%
10 half-lives1/1024~0.1%~99.9%

Half-Lives of Common Radioactive Elements

  • Carbon-14: 5,730 years - Used extensively in radiocarbon dating of archaeological samples
  • Uranium-238: 4.468 billion years - The most abundant uranium isotope in nature
  • Uranium-235: 703.8 million years - The fissile isotope used in nuclear reactors and weapons
  • Plutonium-239: 24,100 years - Used in nuclear weapons and as reactor fuel
  • Cobalt-60: 5.27 years - Widely used in medical radiation therapy and industrial radiography
  • Iodine-131: 8.02 days - Used in thyroid cancer treatment and medical imaging
  • Technetium-99m: 6 hours - The most widely used medical radioisotope for diagnostic imaging
  • Polonium-210: 138.4 days - Historical use in nuclear weapons and alleged poisoning cases

Activity and the Decay Constant

The activity (A) of a radioactive sample measures how many decays occur per second:

A = λN

Activity is measured in Becquerel (Bq), where 1 Bq = 1 decay per second. The older unit is Curie (Ci), where 1 Ci = 3.7 × 10^10 Bq.

The relationship between decay constant and half-life:

λ = ln(2) / t1/2 = 0.693 / t1/2

Real-World Applications

  • Archaeological Dating: Carbon-14 dating allows scientists to determine the age of organic materials up to about 50,000 years old by measuring the remaining C-14 content
  • Medical Treatment: Radioisotopes with specific half-lives are used for targeted cancer therapy, diagnostic imaging, and sterilizing medical equipment
  • Nuclear Power: Understanding half-life helps in calculating fuel consumption, waste management, and reactor safety
  • Geological Dating: Uranium-lead dating is used to determine the age of Earth and geological formations billions of years old
  • Drug Metabolism: The concept of half-life is used in pharmacology to understand how drugs are metabolized and eliminated from the body
  • Environmental Science: Tracking radioactive isotopes in the environment to monitor nuclear accidents and fallout

Important Concept: Radioactive decay is a random process - we cannot predict when any particular atom will decay. However, the statistical behavior of large numbers of atoms is completely predictable. This is known as the law of large numbers in statistics, and it makes half-life calculations extremely reliable for practical applications.