A powder pattern of iron

PHYSICS · Multi-part · Fermi University Physics · Condensed Matter, Materials & Soft Matter · Crystal structure, bonding and diffraction · Crystal structure, bonding and diffraction

Condensed Matter Physics, Ch Diffraction: how a structure is actually measured

Problem

A powder pattern of iron, taken with Cu Kα1\alpha_1 X-rays (λ=1.5406 A˚\lambda=1.5406\,\mathrm{\mathring{A}}), shows six lines at 2θ=44.672\theta=44.67, 65.0265.02, 82.3382.33, 98.9498.94, 116.38116.38 and 137.15137.15 degrees. Iron's measured density is ρ=7.87 g cm−3\rho=7.87\,\mathrm{g\,cm^{-3}} and its molar mass is Mmol=55.85 g mol−1M_{\rm mol}=55.85\,\mathrm{g\,mol^{-1}}. ((a)) Find sin⁡2θ\sin^2\theta for each line and show that their ratios alone cannot distinguish a body-centred cubic lattice from a simple cubic one. ((b)) Using the density, decide which lattice iron actually has, and find its lattice constant aa to four figures.

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