Key Takeaways — Chapter 1
Core Concepts
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The Rutherford scattering cross section for Coulomb scattering of a charge $z_1 e$ from a point charge $z_2 e$ at kinetic energy $T$ is: $$\frac{d\sigma}{d\Omega} = \left(\frac{a}{2}\right)^2 \frac{1}{\sin^4(\theta/2)}, \quad a = \frac{k z_1 z_2 e^2}{2T}$$ The $\sin^{-4}(\theta/2)$ angular dependence was confirmed by Geiger and Marsden and revealed the nuclear atom.
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The neutron was discovered by Chadwick in 1932 via the reaction ${}^{9}\text{Be}(\alpha,n){}^{12}\text{C}$, by analyzing recoil kinematics. The neutron mass $m_n = 939.565\,\text{MeV}/c^2$ is slightly greater than the proton mass $m_p = 938.272\,\text{MeV}/c^2$.
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Nuclear notation: A nuclide ${}^{A}_{Z}\text{X}_N$ is specified by $Z$ (protons), $N$ (neutrons), and $A = Z + N$ (mass number). Isotopes share $Z$; isotones share $N$; isobars share $A$.
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The chart of nuclides maps all ~3,300 known nuclides on an $N$–$Z$ grid. The valley of stability bends toward $N > Z$ for heavy nuclei. Only ~252 nuclides are truly stable.
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Magic numbers: $2, 8, 20, 28, 50, 82, 126$. Nuclei with magic $Z$ or $N$ show enhanced stability (more stable isotopes/isotones, large separation energies). Doubly magic nuclei (${}^{4}\text{He}$, ${}^{16}\text{O}$, ${}^{40}\text{Ca}$, ${}^{48}\text{Ca}$, ${}^{208}\text{Pb}$) are exceptionally stable.
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Nuclear radius and density saturation: $$R = r_0 A^{1/3}, \quad r_0 \approx 1.21\,\text{fm}$$ Because $V \propto A$, nuclear density is approximately constant: $\rho \approx 0.16\,\text{nucleons/fm}^3 \approx 2.3 \times 10^{17}\,\text{kg/m}^3$. This saturation implies the nuclear force is short-ranged.
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Binding energy (the threshold concept of this chapter): $$B(A,Z) = \left[Z m_p + N m_n - M(A,Z)\right]c^2$$ Binding energy is the energy required to disassemble the nucleus — not energy stored inside it. More tightly bound nuclei have less mass per nucleon.
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The binding energy per nucleon curve peaks near ${}^{62}\text{Ni}$ ($B/A = 8.795\,\text{MeV}$) and decreases for both lighter and heavier nuclei. This single curve explains why: - Fusion of light nuclei releases energy (moving up the curve from the left) - Fission of heavy nuclei releases energy (moving up the curve from the right)
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Separation energies $S_n$ and $S_p$ measure the binding of the last neutron or proton. Sharp drops at magic numbers provide direct evidence for nuclear shell closures.
Essential Numbers to Remember
| Quantity | Value |
|---|---|
| $ke^2 = e^2/(4\pi\epsilon_0)$ | $1.44\,\text{MeV}\cdot\text{fm}$ |
| Proton mass $m_p$ | $938.272\,\text{MeV}/c^2 = 1.007276\,\text{u}$ |
| Neutron mass $m_n$ | $939.565\,\text{MeV}/c^2 = 1.008665\,\text{u}$ |
| $1\,\text{u}$ (atomic mass unit) | $931.494\,\text{MeV}/c^2$ |
| Nuclear radius parameter $r_0$ | $\approx 1.21\,\text{fm}$ |
| Nuclear saturation density | $\approx 0.16\,\text{nucleons/fm}^3$ |
| Peak $B/A$ (${}^{62}\text{Ni}$) | $8.795\,\text{MeV/nucleon}$ |
| $B/A$ for ${}^{4}\text{He}$ | $7.074\,\text{MeV/nucleon}$ |
| $B/A$ for ${}^{238}\text{U}$ | $7.570\,\text{MeV/nucleon}$ |
| Magic numbers | 2, 8, 20, 28, 50, 82, 126 |