Crystal structures and Miller indices

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)?

  1. AAbout 0.68
  2. BAbout 0.74
  3. CAbout 0.52
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Answer: B. About 0.74

In FCC, atoms touch along the face diagonal, so √2a = 4r, that is, a = 2√2r. With 4 atoms per unit cell, the packing factor is 4 × (4/3)πr³ / (2√2r)³ = π/(3√2) ≈ 0.74. About 0.68 is the BCC value (atoms touch along the body diagonal, a = 4r/√3, 2 atoms), and about 0.52 is the SC value (a = 2r, 1 atom, π/6). HCP with the ideal c/a also reaches 0.74 and is the other close-packed structure alongside FCC. Note that a high packing factor does not mean that each individual interstitial site is large.

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More Crystal structures and Miller indices questions

  1. 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.
  2. Copper has the FCC structure with a lattice parameter of 0.3615 nm and a molar mass of 63.55 g/mol. Taking Avogadro's number as 6.022×10²³ mol⁻¹, which value is closest to the calculated density of copper?
  3. If the lattice parameter of α-iron (BCC) is 0.2866 nm, which value is closest to the atomic radius in the hard-sphere model?
  4. In a cubic crystal, a plane intercepts the x axis at 1a and the y axis at 2a, and is parallel to the z axis. What are its Miller indices?
  5. Which correctly pairs the close-packed planes and close-packed directions of an FCC metal?