Chap 42: Nuclear Physics#
Sections#
Sec |
Topic |
|---|---|
42-1 |
|
42-2 |
|
42-3 |
|
42-4 |
|
42-5 |
|
42-6 |
|
42-7 |
|
42-8 |
Review & Summary#
- Discovering the Nucleus#
Rutherford scattering of alpha particles from thin metal foils showed that the atom has a small, dense, positively charged nucleus. Most alpha particles pass through with small deflection; the few large-angle scatterings indicate a compact core containing most of the mass.
- Some Nuclear Properties#
A nucleus has \(Z\) protons and \(N\) neutrons. The mass number is \(A = Z + N\). The atomic mass unit is \(1\,\mathrm{u} = 931.5\,\mathrm{MeV}/c^2\). The binding energy \(E_b\) is the energy required to separate the nucleus into its nucleons:
(432)#\[ E_b = (\Delta m)c^2 \]where \(\Delta m\) is the mass defect (difference between the sum of nucleon masses and the nuclear mass). The semi-empirical mass formula describes how \(E_b\) varies with \(A\) and \(Z\).
- Radioactive Decay#
The number \(N\) of undecayed nuclei decreases exponentially with time:
(433)#\[ N = N_0 e^{-\lambda t} \]where \(\lambda\) is the decay constant. The half-life is \(T_{1/2} = (\ln 2)/\lambda = 0.693/\lambda\). The activity (decay rate) is \(R = \lambda N = -dN/dt\), measured in becquerels (Bq; 1 Bq = 1 decay/s).
- Alpha Decay#
A nucleus emits an alpha particle (\(^4\mathrm{He}\) nucleus). The decay energy \(Q\) is the total kinetic energy released. Quantum tunneling through the Coulomb barrier explains how alpha particles escape despite having energy less than the barrier height.
- Beta Decay#
Beta-minus decay: \(n \to p + e^- + \bar{\nu}_e\). Beta-plus decay: \(p \to n + e^+ + \nu_e\). Electron capture: \(p + e^- \to n + \nu_e\). The neutrino (or antineutrino) is required to conserve energy, momentum, and lepton number.
- Radioactive Dating#
Carbon-14 dating: Living organisms maintain a ratio \(^{14}\mathrm{C}/^{12}\mathrm{C}\); after death, \(^{14}\mathrm{C}\) decays (half-life 5730 years) and the ratio decreases. Other isotopes (e.g., uranium series) date older materials.
- Measuring Radiation Dosage#
Absorbed dose: gray (Gy) = 1 J/kg of energy deposited. Equivalent dose: sievert (Sv) = Gy × RBE (relative biological effectiveness). Activity: becquerel (Bq) = 1 decay/s.
- Nuclear Models#
Liquid-drop model: treats the nucleus as an incompressible fluid; explains fission and the semi-empirical mass formula. Shell model: nucleons occupy orbitals; explains magic numbers (2, 8, 20, 28, 50, 82, 126) and nuclear spin.