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).
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 has protons and neutrons. The mass of a nucleus is smaller than the sum of its free nucleons; this mass defect appears as binding energy via , with .
Worked example (helium-4, using atomic masses):
Binding energy per nucleon rises steeply for light nuclei and peaks near and (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 ; heavier stable nuclei need extra neutrons ( 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 , , , and are especially stable.
- Every element beyond bismuth () has only radioactive isotopes.
Decay Modes
| Mode | Emission | Change in , | Typical Parent | Stopped By |
|---|---|---|---|---|
| Alpha | nucleus | , | Heavy nuclei (, ) | A sheet of paper or the outer layer of skin |
| Beta-minus | Electron and antineutrino () | , | Neutron-rich (, , ) | A few millimetres of aluminium or plastic |
| Positron | Positron and neutrino () | , | Proton-rich (, ); needs at least 1.022 MeV | Annihilates with electrons, giving two 511 keV photons |
| Electron capture | Inner electron absorbed; X-rays emitted | , | Proton-rich ( in part, ) | — |
| Gamma / isomeric transition | High-energy photon | No change | Excited states (, 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 :
- Number of alpha decays: , lowering by 16 to 76
- Number of beta-minus decays:
Nuclear Reactions: Transmutation, Fission, and Fusion
Balance nuclear equations by conserving mass number and charge.
- Rutherford's transmutation (1919):
- Fission: , releasing about 200 MeV per fission. The extra neutrons can sustain a chain reaction above the critical mass.
- Fusion: , 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:
Activity is measured in becquerels ( decay per second) or curies (). Absorbed dose is in grays (), and equivalent dose, which weights radiation type, is in sieverts. Section 10.1 applies these equations to radiocarbon dating.
Detection and Radioanalytical Methods
| Detector | Principle | Best For |
|---|---|---|
| Geiger-Muller tube | Gas ionization avalanche | Counting and surveys; no energy information |
| NaI(Tl) scintillator | Light flashes read by a photomultiplier | Efficient gamma counting with moderate energy resolution |
| High-purity germanium (HPGe) | Electron-hole pairs in a semiconductor | High-resolution gamma spectrometry |
| Liquid scintillation counting | Sample dissolved in a scintillator cocktail | Low-energy beta emitters (, ) |
Isotope Dilution
Add a known mass of tracer with specific activity (activity per mass) to the sample, mix, isolate any pure portion of the analyte, and measure its specific activity :
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 , where is the capture cross-section and 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 , , and follow reaction pathways and metabolism. Radiometric dating uses known half-lives: (5730 y) for organic materials up to about 50,000 years, and the / or / systems for rocks.
Thorium-232 (Z = 90) undergoes alpha decay. What is the daughter nuclide?
Thorium-228 (Z = 90)
Actinium-232 (Z = 89)
Radium-228 (Z = 88)
Uranium-236 (Z = 92)
How many alpha and beta-minus decays convert uranium-238 (Z = 92) into lead-206 (Z = 82)?
8 alpha and 10 beta-minus
6 alpha and 8 beta-minus
10 alpha and 4 beta-minus
8 alpha and 6 beta-minus
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?
25.0 mg
0.16 mg
23.0 mg
12.5 mg
Sections you finish are checked off in the contents.