E.1.9 (HL)—Closest approach

Syllabus
First assessment 2025
Objective
Level
HL

Calculate Closest Approach

HL only

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=8.0×1013JE_k=5.0\,\mathrm{MeV}=8.0\times10^{-13}\,\mathrm{J}, qα=2eq_\alpha=2e and qN=79eq_N=79e, rmin=k(2e)(79e)/Ek=4.5×1014mr_{\min}=k(2e)(79e)/E_k=4.5\times10^{-14}\,\mathrm{m}. 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 qαq_\alpha and qnucleusq_{nucleus}. Also do not leave energy in MeV while using kk in SI units.

E.1.9 (HL) Exam Analysis

HL only

Assessment in practice

2–4 marks
How it is assessed

Questions calculate r_min for alpha particles incident on gold, sometimes from accelerating potential or a stated kinetic energy.

Command terms

Calculate / Determine

What earns marks

Convert the particle energy to joules when using SI constants, use both interacting charges, and state the closest-approach relation from energy conservation.

Watch for

Using only the gold-nucleus charge, missing the alpha charge, or mixing MeV with joules.

Retrieve the HL Atomic Model

HL only

Retrieve the HL extensions

Use R=R0A1/3R=R_0A^{1/3} 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/n2eVE_n=-13.6/n^2\,\mathrm{eV}, and allowed angular momentum mvr=nh/(2π)mvr=nh/(2\pi) produces discrete orbits and energies.