Back/Chemistry: Atoms First 2e
Section 20.312 Key Terms

Radioactive Decay

Learning Objectives
  • Identify decay modes and their changes to mass number and atomic number
  • Calculate remaining isotope amount, activity, half-life, or elapsed time
  • Explain radioactive decay series and radiometric dating

Core Concepts & Principles

Radioactive decay is the spontaneous change of an unstable parent nuclide into a daughter nuclide, which may be stable or may decay again. Decay often brings a nucleus closer to the band of stability.

Decay Modes

ModeWhat happensChange in AAChange in ZZ
Alpha (α) decayEmits a helium nucleus, 24He^4_2\text{He}−4−2
Beta-minus (β⁻) decayA neutron becomes a proton and emits an electron, −10e^0_{-1}\text{e}0+1
Positron (β⁺) emissionA proton becomes a neutron and emits a positron, +10e^0_{+1}\text{e}0−1
Electron captureA proton captures an inner-shell electron and becomes a neutron0−1
Gamma (γ) emissionAn excited nucleus loses energy as a photon, 00γ^0_0\gamma00

Neutron-rich nuclei tend to undergo beta-minus decay; proton-rich nuclei may undergo positron emission or electron capture. Very heavy nuclei commonly undergo alpha decay. Gamma emission often follows another decay that leaves the daughter excited. Electron capture can be followed by X-rays as electrons refill the vacancy. Beta decay and electron capture also involve neutrinos or antineutrinos; introductory nuclear equations usually omit these because they have A=0A=0 and charge 0.

In a radioactive decay series, one daughter becomes the next parent. For example, uranium-238 passes through several alpha and beta decays before reaching stable lead-206.

First-Order Decay and Half-Life

Decay follows first-order kinetics: activity is λN\lambda N, where NN counts the remaining nuclei of the radioactive isotope and λ\lambda is its decay constant. The half-life, t1/2t_{1/2}, is the time for half those nuclei to decay. Each half-life halves their amount; it does not remove half the entire physical sample, because daughter atoms remain.

Half-lives range from fractions of a second to billions of years and are characteristic of each isotope under ordinary conditions. After kk half-lives, the remaining fraction is (1/2)k(1/2)^k. Amount, concentration, and activity ratios follow the same decay relation for the same isotope with consistent measurement conditions.

Radiometric Dating

Radiometric dating uses known decay rates and parent/daughter amounts to estimate age. Choose an isotope with a half-life appropriate to the timescale, and account for any daughter material present initially and later movement or contamination of isotopes. Uranium-238 (t1/2≈4.5×109t_{1/2}\approx4.5\times10^9 years) can date old rocks through its decay to lead-206.

Radiocarbon dating applies to once-living material. Cosmic-ray neutrons produce carbon-14 from atmospheric nitrogen:

714N+01n→614C+11H^{14}_7\text{N} + ^1_0\text{n} \rightarrow ^{14}_6\text{C} + ^1_1\text{H}

Carbon-14 enters CO₂ and living organisms through photosynthesis and food chains. Living organisms continually exchange carbon; after death, exchange stops and C-14 decays (t1/2=5730t_{1/2}=5730 years), while stable C-12 remains. Compare the sample's C-14/C-12 ratio or activity per gram of carbon with a suitable reference. Atmospheric changes require calibration. The useful range is roughly up to 50,000 years; very old samples contain too little C-14 for reliable measurement. Other isotopes suit older geological samples.

The Same Fraction Decays in Each Equal Time Interval

Decay removes a constant fraction, not a constant number of nuclei. A smaller sample has lower activity but the same half-life.

Problem-Solving Routines & Methods

Half-Life and Decay Constant
t1/2=ln⁡2λ=0.693λt_{1/2} = \frac{\ln 2}{\lambda} = \frac{0.693}{\lambda}
Variables & Constants
t1/2t_{1/2}=half-life;
λ\lambda=decay constant in inverse time units
Integrated Decay Law
Nt=N0e−λt,ln⁡(NtN0)=−λtN_t = N_0 e^{-\lambda t}, \qquad \ln\left(\frac{N_t}{N_0}\right)=-\lambda t
Variables & Constants
N0N_0=initial nuclei count;
NtN_t=remaining count;
tt=elapsed time
Finding Age or Elapsed Time
t=ln⁡(N0/Nt)λt = \frac{\ln(N_0/N_t)}{\lambda}

The same formula works with initial and current activities of the same isotope.

Solving Decay and Dating Problems
  1. 1
    Identify the initial and remaining isotope amounts or activities, and form a ratio using matching units.
  2. 2
    Find the decay constant from the half-life. Use the same time units for half-life and elapsed time.
  3. 3
    Use repeated halving for a whole number of half-lives; otherwise use the exponential or logarithmic decay equation.
  4. 4
    Check that a decaying amount decreases and that the calculated elapsed time is positive.

Practice & Concept Checks

Concept Check
An isotope has a half-life of 2.0 hours. What fraction remains after 6.0 hours?
Concept Check
Once-living material has one-quarter of its reference C-14 activity. Estimate its age before calibration.
Concept Check
How do beta-minus decay and positron emission change atomic number?

Key Terms & Vocabulary

alpha (α) decayRadioactive Decay
loss of an alpha particle during radioactive decay
beta (β) decayRadioactive Decay
breakdown of a neutron into a proton, which remains in the nucleus, and an electron, which is emitted as a beta particle
daughter nuclideRadioactive Decay
nuclide produced by the radioactive decay of another nuclide; may be stable or may decay further
electron captureRadioactive Decay
combination of a core electron with a proton to yield a neutron within the nucleus
gamma (γ) emissionRadioactive Decay
decay of an excited-state nuclide accompanied by emission of a gamma ray
half-life (t₁/₂)Radioactive Decay
time required for half of the atoms in a radioactive sample to decay
parent nuclideRadioactive Decay
unstable nuclide that changes spontaneously into another (daughter) nuclide
positron emissionRadioactive Decay
(also, β⁺ decay) conversion of a proton into a neutron, which remains in the nucleus, and a positron, which is emitted
radioactive decayRadioactive Decay
spontaneous decay of an unstable nuclide into another nuclide
radioactive decay seriesRadioactive Decay
chains of successive disintegrations (radioactive decays) that ultimately lead to a stable end-product
radiocarbon datingRadiometric Dating
highly accurate means of dating objects 30,000–50,000 years old that were derived from once-living matter; achieved by calculating the ratio of  614C:  612C{}_{\,6}^{14}\text{C}\text{:}\,{}_{\,6}^{12}\text{C} in the object vs. the ratio of  614C:  612C{}_{\,6}^{14}\text{C}\text{:}\,{}_{\,6}^{12}\text{C} in the present-day atmosphere
radiometric datingRadiometric Dating
use of radioisotopes and their properties to date the formation of objects such as archeological artifacts, formerly living organisms, or geological formations