Dashboard/Learning Hub/Physics HL/Chapter 22/22.5 Electron Diffraction, Bragg Geometry, and Quantised Orbits

Physics HL · Chapter 22: Quantum Physics

22.5 Electron Diffraction, Bragg Geometry, and Quantised Orbits

Link Davisson-Germer diffraction evidence to crystal path difference and Bohr standing-wave orbit interpretation.

Estimated time: 42 minutes

Davisson-Germer as Direct Matter-Wave Evidence

Electron beams scattered by crystalline nickel show intensity maxima at specific angles, exactly like wave interference from layered scattering centers. These angular peaks cannot be explained by random particle bounce distributions alone. They match path-difference conditions for constructive interference when interplanar geometry and de Broglie wavelength are combined.

Experimentally, once kinetic energy sets electron wavelength through h/p, measured peak angles can be predicted. Or equivalently, measured angles can be used to infer wavelength and compared with de Broglie prediction. Agreement between these independent routes is what gives strong confidence in matter-wave interpretation.

Bragg Condition for Constructive Interference

2dsinθ=nλ2d\sin\theta = n\lambda

d is layer spacing, theta is scattering geometry angle, n is integer order.

Always run a feasibility check before solving for angle: n lambda/(2d) must be less than or equal to 1. If it exceeds 1, that order is not physically allowed for that wavelength and spacing. This simple inequality is often faster than full trigonometric calculation and prevents impossible results.

Connection to Bohr Orbit Quantisation

2πr=nλ2\pi r = n\lambda

Allowed Bohr-like orbits correspond to standing-wave closure around circumference.

This standing-wave picture provides intuition for why only discrete radii/energies are stable in early quantum models: if circumference does not fit an integer number of wavelengths, destructive self-interference prevents a stationary wave pattern. While full quantum mechanics replaces Bohr orbits with orbitals and wavefunctions, this relation remains a powerful conceptual bridge.

Note

de Broglie + Bragg explains measured diffraction geometry; full wave mechanics is needed for intensities and full atomic structure predictions.

Simulation: Diffraction Profile and Bragg-Order Explorer

Inspect intensity-vs-angle patterns while changing particle type, kinetic energy, spacing, and order to see when constructive peaks exist.

Diffraction Intensity vs Angle

angle (deg)relative intensityBragg condition: 2d sin(theta) = n lambda

A clear diffraction peak requires wavelength comparable to lattice spacing. Heavy particles at the same kinetic energy have shorter de Broglie wavelengths and weaker angular spread.

De Broglie Lambda

0.112 nm

Momentum

5.92e-24 kg m/s

Particle Charge

-e

Bragg Angle

68.903 deg

Electron accelerator view: kinetic energy of 120.000 eV corresponds to acceleration through approximately the same number of volts.

Test Yourself

Why do heavier particles at the same kinetic energy usually produce less obvious diffraction than electrons?