Peierls stress

Peierls stress (or Peierls–Nabarro stress, also known as the lattice friction stress^[1]) is the force (first described by Rudolf Peierls and modified by Frank Nabarro) needed to move a dislocation within a plane of atoms in the unit cell. The magnitude varies periodically as the dislocation moves within the plane. Peierls stress depends on the size and width of a dislocation and the distance between planes. Because of this, Peierls stress decreases with increasing distance between atomic planes. Yet since the distance between planes increases with planar atomic density, slip of the dislocation is preferred on closely packed planes.

Peierls–Nabarro stress proportionality

${\displaystyle \tau _{\mathrm {PN} }\propto Ge^{-2{\pi }W/b}}$

Where:

${\displaystyle W={\frac {d}{1-\nu }}=}$ the dislocation width

${\displaystyle G}$ = shear modulus

${\displaystyle \nu }$ = Poisson's ratio

${\displaystyle b}$ = slip distance or Burgers vector

${\displaystyle d}$ = interplanar spacing

Yield strength temperature sensitivity

The Peierls stress also relates to the temperature sensitivity of the yield strength of material because it very much depends on both short-range atomic order and atomic bond strength. As temperature increases, the vibration of atoms increases, and thus both peierls stress and yield strength decrease as a result of weaker atomic bond strength at high temperatures.

See also

• Frenkel–Kontorova model