E.1.9 (HL)—Closest approach
- Syllabus
- First assessment 2025
- Objective
- —
- Level
- HL
Use energy conservation
For a head-on alpha particle, the initial kinetic energy is converted into electric potential energy as the particle approaches the positive nucleus. At the turning point, the radial kinetic energy is zero.
Set the energies equal
At the turning point the radial kinetic energy is zero, so the initial kinetic energy equals the electric potential energy of the repulsive alpha-particle–nucleus system. Both positive charges must be included.
E_{k,\mathrm{initial}}=\frac{kq_\alpha q_N}{r_{\min}}\quad\Rightarrow\quad r_{\min}=\frac{kq_\alpha q_N}{E_{k,\mathrm{initial}}}
Worked example — alpha particle toward gold
For Ek=5.0MeV=8.0×10−13J, qα=2e and qN=79e, rmin=k(2e)(79e)/Ek=4.5×10−14m. This is a turning-point distance, not automatically the nuclear radius.
Check the turning point
At closest approach the alpha particle has momentarily stopped moving toward the nucleus, then reverses. A larger initial kinetic energy gives a smaller closest-approach distance.
Common trap
Do not use the charge of gold alone: the interaction contains both qα and qnucleus. Also do not leave energy in MeV while using k in SI units.
Questions calculate r_min for alpha particles incident on gold, sometimes from accelerating potential or a stated kinetic energy.
Calculate / Determine
Convert the particle energy to joules when using SI constants, use both interacting charges, and state the closest-approach relation from energy conservation.
Using only the gold-nucleus charge, missing the alpha charge, or mixing MeV with joules.
Retrieve the HL extensions
Use R=R0A1/3 for nuclear scale, recognise when high-energy scattering exceeds the electrostatic model, and use energy conservation for head-on closest approach.
Retrieve the Bohr model
Hydrogen levels obey En=−13.6/n2eV, and allowed angular momentum mvr=nh/(2π) produces discrete orbits and energies.