A materials scientist at a Wellington laboratory studies the surface of a new alloy using low-energy electron diffraction. Electrons are accelerated from rest through a potential difference
V and strike the crystal surface at normal incidence. The surface atoms are arranged in parallel rows a distance
d apart, and they act like a reflection grating: back-scattered electrons produce strong maxima at angles
θ from the normal given by
dsinθ=nλ, where
n is the order. The electron speeds are non-relativistic. The scientist measures the angle
θ1 of the first-order maximum at several accelerating voltages:
V (V): 50.0, 80.0, 120, 180, 250
θ1 (∘): 44.3, 33.1, 26.6, 21.7, 17.9