Diffraction by Organized Layers — Question 3

Section 36-9 · Physics pages 6016–6017

Question 3 A cubic lattice parameter predicts another plane-family peak A cubic crystal obeys dhkl = a/ √ h2 + k2 + l2. With wavelength 0.154 nm, its first-order (111) reflection occurs at scattering angle 2θ = 60.0◦. Assume both (111) and (200) are allowed reflections. a Schematic; labels, not drawing lengths, specify the data. (a) Infer the cubic lattice parameter a. (b) Predict the first-order (200) scattering angle.
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Question 3 - Solution A cubic lattice parameter predicts another plane-family peak a (a) Method and calculation θ111 = 30◦, d111 = λ/(2 sin 30◦) = 0.154 nm. a = √ 3d111 = 0.266736 nm . (b) Interpretation and further calculation d200 = a/2, sin θ200 = λ/(2d200) = 1/ √ 3. 2θ200 = 70.5288◦. Physical check Different plane families are labeled by their Miller indices; they need not be successive diffraction orders of a single spacing.

Question 3

A cubic lattice parameter predicts another plane-family peak

A cubic crystal obeys dhkl=a/h2+k2+l2d_{hkl}=a/\sqrt{h^2+k^2+l^2}. With wavelength 0.154nm0.154\,\mathrm{nm}, its first-order (111) reflection occurs at scattering angle 2θ=60.0∘2\theta=60.0^\circ. Assume both (111) and (200) are allowed reflections.

Diagram shown in the original SVG worksheet.

  1. Infer the cubic lattice parameter a.

  2. Predict the first-order (200) scattering angle.

Question 3 - Solution

A cubic lattice parameter predicts another plane-family peak

Diagram shown in the original SVG worksheet.

(a) Method and calculation

θ111=30∘,d111=λ/(2sin⁡30∘)=0.154nm.\theta_{111}=30^\circ,\quad d_{111}=\lambda/(2\sin30^\circ)=0.154\,\mathrm{nm}.a=3d111=0.266736nm.\boxed{a=\sqrt3d_{111}=0.266736\,\mathrm{nm}}.

(b) Interpretation and further calculation

d200=a/2,sin⁡θ200=λ/(2d200)=1/3.d_{200}=a/2,\quad\sin\theta_{200}=\lambda/(2d_{200})=1/\sqrt3.2θ200=70.5288∘.\boxed{2\theta_{200}=70.5288^\circ}.

Physical check

Different plane families are labeled by their Miller indices; they need not be successive diffraction orders of a single spacing.