In crystallography, atomic packing factor (APF), packing efficiency or packing fraction is the fraction of volume in a crystal structure that is occupied by constituent particles. It is dimensionless and always less than unity. In atomic systems, by convention, the APF is determined by assuming that atoms are rigid spheres. The radius of the spheres is taken to be the maximal value such that the atoms do not overlap. For onecomponent crystals (those that contain only one type of particle), the packing fraction is represented mathematically by

\mathrm{APF} = \frac{N_\mathrm{particle} V_\mathrm{particle}}{V_\mathrm{unit cell}}
where N_{particle} is the number of particles in the unit cell, V_{particle} is the volume of each particle, and V_{unit cell} is the volume occupied by the unit cell. It can be proven mathematically that for onecomponent structures, the most dense arrangement of atoms has an APF of about 0.74 (see Kepler conjecture), obtained by the closepacked structures. For multiplecomponent structures, the APF can exceed 0.74.
Contents

Single component crystal structures 1

Bodycentered cubic 1.1

Hexagonal closepacked 1.2

See also 2

References 3

Further reading 4
Single component crystal structures
Common sphere packings taken on by atomic systems are listed below with their corresponding packing fraction.
The majority of metals take on either the hcp, ccp or bcc structure.^{[2]}
Bodycentered cubic
BCC structure
The primitive unit cell for the bodycentered cubic crystal structure contains several fractions taken from nine atoms: one on each corner of the cube and one atom in the center. Because the volume of each of the eight corner atoms is shared between eight adjacent cells, each BCC cell contains the equivalent volume of two atoms (one central and one on the corner).
Each corner atom touches the center atom. A line that is drawn from one corner of the cube through the center and to the other corner passes through 4r, where r is the radius of an atom. By geometry, the length of the diagonal is a√3. Therefore, the length of each side of the BCC structure can be related to the radius of the atom by

a = \frac{4r}{\sqrt{3}}.
Knowing this and the formula for the volume of a sphere, it becomes possible to calculate the APF as follows:

\mathrm{APF} = \frac{N_\mathrm{atoms} V_\mathrm{atom}}{V_\mathrm{crystal}} = \frac{2 (4/3)\pi r^3}{(4r/\sqrt{3})^3}



= \frac{\pi\sqrt{3}}{8} \approx 0.68.\,\!
Hexagonal closepacked
HCP structure
For the hexagonal closepacked structure the derivation is similar. Here the unit cell (equivalent to 3 primitive unit cells) is a hexagonal prism containing six atoms. Let a be the side length of its base and c be its height. Then:

a = 2r

c = \sqrt{\frac{2}{3}}(4r).
It is then possible to calculate the APF as follows:

\mathrm{APF} = \frac{N_\mathrm{atoms}\cdot V_\mathrm{atom}}{V_\mathrm{crystal}} = \frac{6\cdot (4/3)\pi r^3})(4r)} = \frac{6 (4/3)\pi r^3})(16r^3)}



= \frac{\pi}{\sqrt{18}} \approx 0.74.\,\!
See also
References

^ ^{a} ^{b} ^{c} ^{d} Ellis, Arthur B. [et al.] (1995). Teaching general chemistry : a materials science companion (3. print ed.). Washington: American Chemical Society.

^ Moore, Lesley E. Smart; Elaine A. (2005). Solid state chemistry : an introduction (3. ed.). Boca Raton, Fla. [u.a.]: Taylor & Francis, CRC. p. 8.
Further reading

Schaffer, Saxena, Antolovich, Sanders, and Warner (1999). The Science and Design of Engineering Materials (Second ed.). New York: WCB/McGrawHill. pp. 81–88.

Callister, W. (2002). Materials Science and Engineering (Sixth ed.). San Francisco: John Wiley and Sons. pp. 105–114.
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