under appropriate conditions, dislocation glide can appear not only in comp
act crystal planes which are optimum for its realization, but also in other
types of nan-compact (NCI planes. The interest in a more systematical know
ledge of this mechanism was increased in connection with its importance in
modern metallic and inter-metallic materials, but the phenomenon was also w
idely investigated in pure metals. This paper tries to give an overview of
a published knowledge on the non-compact dislocation glide mostly in metall
ic materials. It starts from model ideas and illustrates their realization
by characteristic performances of the non-compact glide in experiments.
As mechanisms of the NC glide, the Peierls mechanism and the locking-unlock
ing combination can be accepted. In fee metals, the NC glide can appear in
several types of crystal planes, the intensity of its participation in stra
ining, beside the glide in the compact planes, depends on the stacking faul
t energy and is a function of temperature. As thermally activated process,
NC glide is characterized by an activation energy which is higher than the
activation energy of lattice diffusion. In hcp metals, a pure NC glide can
be realized. Deformation stresses of non-basal systems depend on the disloc
ation core structure and the stacking fault energy. In intermetallics, the
NC glide assists in the motion of superdislocations and dislocations by act
ing in a cross slip between a compact and a NC plane. A similar participati
on of the NC glide is observed also in superalloys. The deformation stress
anomaly at higher temperatures might be connected with a realization of the
NC glide.