Editing Crystal (section)

== Special properties from anisotropy ==
{{See also|Crystal optics}}
Crystals can have certain special electrical, optical, and mechanical properties that [[glass]] and [[polycrystal]]s normally cannot. These properties are related to the [[anisotropy]] of the crystal, i.e. the lack of rotational symmetry in its atomic arrangement. One such property is the [[piezoelectric effect]], where a voltage across the crystal can shrink or stretch it. Another is [[birefringence]], where a double image appears when looking through a crystal. Moreover, various properties of a crystal, including [[electrical conductivity]], [[electrical permittivity]], and [[Young's modulus]], may be different in different directions in a crystal. For example, [[graphite]] crystals consist of a stack of sheets, and although each individual sheet is mechanically very strong, the sheets are rather loosely bound to each other. Therefore, the mechanical strength of the material is quite different depending on the direction of stress.

Not all crystals have all of these properties. Conversely, these properties are not quite exclusive to crystals. They can appear in [[glass]]es or [[polycrystal]]s that have been made [[anisotropic]] by [[Work hardening|working]] or [[stress (mechanics)|stress]]—for example, [[photoelasticity|stress-induced birefringence]].