4.6 Nuclear Chemistry: Stability, Decay, Transmutation, and Radioanalytical Methods

Key Takeaways

  • Nuclear binding energy comes from the mass defect (1 u = 931.494 MeV); helium-4 is bound by about 28.3 MeV, and binding energy per nucleon peaks near iron and nickel at about 8.8 MeV.

  • Alpha decay lowers A by 4 and Z by 2; beta-minus decay raises Z by 1; positron emission and electron capture lower Z by 1; gamma emission changes neither.

  • Uranium-238 decays to lead-206 through 8 alpha and 6 beta-minus decays, because the mass number falls by 32 and the atomic number by 10.

  • Radioactive decay is first order, so activity A = lambda N and the half-life is ln 2 / lambda regardless of the amount present.

  • Isotope dilution finds an unknown amount from the drop in specific activity: m_x = m_s (S_s / S_m - 1).

Last updated: October 2026

4.6 Nuclear Chemistry: Stability, Decay, Transmutation, and Radioanalytical Methods

Quick Answer: Nuclear chemistry is a 10-item area of the Inorganic Chemistry TOS. Analytical Chemistry adds radioanalytical methods. Expect to balance nuclear equations, predict decay modes from neutron-to-proton ratios, compute binding energies from mass defects, count steps in decay series, and handle first-order decay, isotope dilution, and activation analysis.


The Nucleus and Binding Energy

A nuclide ZAX^{A}_{Z}X has ZZ protons and N=A−ZN = A - Z neutrons. The mass of a nucleus is smaller than the sum of its free nucleons; this mass defect Δm\Delta m appears as binding energy via E=Δm c2E = \Delta m\,c^2, with 1 u=931.494 MeV1\text{ u} = 931.494\text{ MeV}.

Worked example (helium-4, using atomic masses):

Δm=2(1.007825)+2(1.008665)−4.002603=0.030377 u\Delta m = 2(1.007825) + 2(1.008665) - 4.002603 = 0.030377\text{ u}

EB=0.030377×931.494=28.30 MeV(7.07 MeV per nucleon)E_B = 0.030377 \times 931.494 = 28.30\text{ MeV} \quad (7.07\text{ MeV per nucleon})

Binding energy per nucleon rises steeply for light nuclei and peaks near 56Fe^{56}Fe and 62Ni^{62}Ni (about 8.8 MeV). Fusion of light nuclei and fission of heavy nuclei both release energy by moving toward that peak.

The Band of Stability

  • Stable light nuclei have N/Z≈1N/Z \approx 1; heavier stable nuclei need extra neutrons (N/Z≈1.5N/Z \approx 1.5 near lead).
  • Nuclei with even numbers of both protons and neutrons are most often stable. Magic numbers (2, 8, 20, 28, 50, 82, 126) give extra stability, so 4He^{4}He, 16O^{16}O, 40Ca^{40}Ca, and 208Pb^{208}Pb are especially stable.
  • Every element beyond bismuth (Z>83Z > 83) has only radioactive isotopes.

Decay Modes

ModeEmissionChange in AA, ZZTypical ParentStopped By
Alpha24He^{4}_{2}He nucleusA−4A - 4, Z−2Z - 2Heavy nuclei (238U^{238}U, 226Ra^{226}Ra)A sheet of paper or the outer layer of skin
Beta-minusElectron and antineutrino (n→pn \rightarrow p)AA, Z+1Z + 1Neutron-rich (14C^{14}C, 3H^{3}H, 131I^{131}I)A few millimetres of aluminium or plastic
PositronPositron and neutrino (p→np \rightarrow n)AA, Z−1Z - 1Proton-rich (18F^{18}F, 11C^{11}C); needs at least 1.022 MeVAnnihilates with electrons, giving two 511 keV photons
Electron captureInner electron absorbed; X-rays emittedAA, Z−1Z - 1Proton-rich (40K^{40}K in part, 55Fe^{55}Fe)—
Gamma / isomeric transitionHigh-energy photonNo changeExcited states (99mTc^{99m}Tc, 140 keV, half-life 6.0 h)Thick lead or concrete

Alpha emitters are relatively harmless outside the body but very damaging when inhaled or ingested, because their energy is deposited over a very short path.

Decay Series

Uranium-238 decays through a chain to stable lead-206. Because only alpha decay changes AA:

  • Number of alpha decays: (238−206)/4=8(238 - 206)/4 = 8, lowering ZZ by 16 to 76
  • Number of beta-minus decays: 82−76=682 - 76 = 6

Nuclear Reactions: Transmutation, Fission, and Fusion

Balance nuclear equations by conserving mass number and charge.

  • Rutherford's transmutation (1919): 714N+24He→817O+11H^{14}_{7}N + ^{4}_{2}He \rightarrow ^{17}_{8}O + ^{1}_{1}H
  • Fission: 92235U+01n→56141Ba+3692Kr+3 01n^{235}_{92}U + ^{1}_{0}n \rightarrow ^{141}_{56}Ba + ^{92}_{36}Kr + 3\,^{1}_{0}n, releasing about 200 MeV per fission. The extra neutrons can sustain a chain reaction above the critical mass.
  • Fusion: 12H+13H→24He+01n^{2}_{1}H + ^{3}_{1}H \rightarrow ^{4}_{2}He + ^{1}_{0}n, releasing 17.6 MeV.

The Q-value of a reaction is the mass difference between reactants and products, times 931.494 MeV per u. A positive Q means energy is released.


Decay Kinetics and Units

Radioactive decay is first order and independent of temperature, pressure, and chemical form:

N=N0e−λt,A=λN,t1/2=ln⁡2λN = N_0 e^{-\lambda t}, \qquad A = \lambda N, \qquad t_{1/2} = \frac{\ln 2}{\lambda}

Activity is measured in becquerels (1 Bq=11\text{ Bq} = 1 decay per second) or curies (1 Ci=3.7×1010 Bq1\text{ Ci} = 3.7 \times 10^{10}\text{ Bq}). Absorbed dose is in grays (1 Gy=1 J/kg1\text{ Gy} = 1\text{ J/kg}), and equivalent dose, which weights radiation type, is in sieverts. Section 10.1 applies these equations to radiocarbon dating.


Detection and Radioanalytical Methods

DetectorPrincipleBest For
Geiger-Muller tubeGas ionization avalancheCounting and surveys; no energy information
NaI(Tl) scintillatorLight flashes read by a photomultiplierEfficient gamma counting with moderate energy resolution
High-purity germanium (HPGe)Electron-hole pairs in a semiconductorHigh-resolution gamma spectrometry
Liquid scintillation countingSample dissolved in a scintillator cocktailLow-energy beta emitters (3H^{3}H, 14C^{14}C)

Isotope Dilution

Add a known mass msm_s of tracer with specific activity SsS_s (activity per mass) to the sample, mix, isolate any pure portion of the analyte, and measure its specific activity SmS_m:

mx=ms(SsSm−1)m_x = m_s\left(\frac{S_s}{S_m} - 1\right)

Recovery need not be complete, because only the ratio of activity to mass is measured.

Neutron Activation Analysis (NAA)

Irradiating a sample with neutrons converts stable nuclei into radioactive ones. Their characteristic gamma rays identify and quantify elements at trace levels. Induced activity is A=Nσϕ(1−e−λtirr)A = N\sigma\phi(1 - e^{-\lambda t_{irr}}), where σ\sigma is the capture cross-section and ϕ\phi the neutron flux. NAA is non-destructive and multi-element, and it is widely used for trace elements in geological, forensic, and environmental samples.

Radiotracers and Dating

Tracers such as 32P^{32}P, 35S^{35}S, and 14C^{14}C follow reaction pathways and metabolism. Radiometric dating uses known half-lives: 14C^{14}C (5730 y) for organic materials up to about 50,000 years, and the 40K^{40}K/40Ar^{40}Ar or 238U^{238}U/206Pb^{206}Pb systems for rocks.

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Predicting the Decay Mode
Test Your Knowledge

Thorium-232 (Z = 90) undergoes alpha decay. What is the daughter nuclide?

A

Thorium-228 (Z = 90)

B

Actinium-232 (Z = 89)

C

Radium-228 (Z = 88)

D

Uranium-236 (Z = 92)

Test Your Knowledge

How many alpha and beta-minus decays convert uranium-238 (Z = 92) into lead-206 (Z = 82)?

A

8 alpha and 10 beta-minus

B

6 alpha and 8 beta-minus

C

10 alpha and 4 beta-minus

D

8 alpha and 6 beta-minus

Test Your Knowledge

To find the amount of an amino acid in a protein hydrolysate, 2.00 mg of the same amino acid labelled with carbon-14 (specific activity 5000 counts/min per mg) is added. A pure portion of the amino acid is isolated and has a specific activity of 400 counts/min per mg. How much amino acid was in the original sample?

A

25.0 mg

B

0.16 mg

C

23.0 mg

D

12.5 mg

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