Crystal structures and Miller indices

In a cubic crystal, which value is closest to the angle between the [100] and [111] directions?

  1. AAbout 45.0°
  2. BAbout 35.3°
  3. CAbout 54.7°
Show answer and explanation

Answer: C. About 54.7°

In cubic crystals, the angle between two directions can be found from the dot product. For [100] and [111], cosθ = (1×1 + 0×1 + 0×1)/(1 × √3) = 1/√3 ≈ 0.577, so θ ≈ 54.7°. About 35.3° is the angle between [110] and [111] (cosθ = 2/√6), and about 45.0° is the angle between [100] and [110]. Because the [hkl] direction is normal to the (hkl) plane in cubic crystals, 54.7° is also the angle between the (100) and (111) planes, familiar as the slope of the {111} sidewalls that appear when (100) silicon is etched in an alkaline solution.

Report an error

Practice this topic Back to topic

Related calculators

More Crystal structures and Miller indices questions

  1. At 912 °C, pure iron transforms from BCC α-iron (lattice parameter 0.2904 nm) to FCC γ-iron (lattice parameter 0.3647 nm). Which correctly describes the change in volume per atom? Both lattice parameters are values at 912 °C.
  2. In a face-centered cubic (FCC) metal, how many atoms touch a given atom at the nearest-neighbor distance (the coordination number)?
  3. What is the net number of atoms in a body-centered cubic (BCC) unit cell?
  4. Treating atoms as hard spheres of equal size, what is the atomic packing factor of the FCC structure (the fraction of the unit-cell volume occupied by atoms)?
  5. Which correctly relates the lattice parameter a and the atomic radius r in the BCC structure? Assume hard-sphere atoms with nearest neighbors in contact.