# Difference between revisions of "Piezoelectricity"

### From Online Dictionary of Crystallography

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== See also == | == See also == | ||

− | + | *[http://www.iucr.org/iucr-top/comm/cteach/pamphlets/18/ An introduction to crystal physics] (Teaching Pamphlet of the ''International Union of Crystallography'') | |

− | [http://www.iucr.org/iucr-top/comm/cteach/pamphlets/18/ An introduction to crystal physics] (Teaching Pamphlet of the ''International Union of Crystallography'') | + | *Section 3.2.2.6 of ''International Tables of Crystallography, Volume A'', 6<sup>th</sup> edition |

− | Section | + | *Section 1.1.4 of ''International Tables of Crystallography, Volume D'' |

− | Section 1.1.4 of ''International Tables of Crystallography, Volume D'' | ||

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[[Category:Physical properties of crystals]]<br> | [[Category:Physical properties of crystals]]<br> |

## Revision as of 16:23, 10 April 2017

Piezoélectricité (*Fr*). Piezoelectrizität (*Ge*). Piezoelectricidad (*Sp*). Piezoelettricità (*It*). 圧電効果 (*Ja*)

## Definition

Piezoelectricity is the property presented by certain materials that exhibit an electric polarization when submitted to an applied mechanical stress such as a uniaxial compression. Conversely, their shape changes when they are submitted to an external electric field; this is the converse piezoelectric effect. The piezoelectric effect and the converse effect are described by third-rank tensors:

- For a small stress, represented by a second-rank tensor,
*T*, the resulting polarization, of components P_{ij}, is given by:_{k}

*P*=

_{k}*d*

_{kij}T_{ij}where *d _{kij}* is a third-rank tensor representing the direct piezoelectric effect.

- For a small applied electric field, of components
*E*, the resulting strain, represented by a second-rank tensor,_{k}*S*, is given by:_{ij}

*S*=

_{ij}*d*+

_{ijk}E_{k}*Q*

_{ijkl}E_{k}E_{l}where the first-order term, *d _{ijk}*, represents the inverse piezoelectric effect and the second-order term,

*Q*, a symmetric fourth-rank tensor, the electrostriction effect. The sense of the strain due to the piezoelectric effect changes when the sign of the applied electric field changes , while that due to electrostriction, a quadratic effect, does not.

_{ijkl}The matrices associated to the coefficients *d _{kij}* and

*d*of the direct and converse piezoelectric effects, respectively, are transpose of one another.

_{kij}## Piezoelectric point groups

The geometric crystal classes for which the piezoelectric effect is possible are determined by symmetry considerations (see Curie laws). They are the non-centrosymmetric classes, with the exception of 432. The 20 piezoelectric crystal classes are therefore:

1, 2, *m*, 222, 2*mm*,
3, 32, 3*m*, 4, [math]{\bar 4}[/math],422, 4*mm*, [math]{\bar 4}[/math]2*m*, 6, [math]{\bar 6}[/math], 622, 6*mm*, [math]{\bar 6}[/math]2*m*,
23, [math]{\bar 4}[/math]3*m*.

Quartz, belonging to geometric crystal class 32, is the most widely used piezoelectric crystal.

## History

It is considerations of symmetry that led the brothers Jacques (1855-1941) and Pierre Curie (1859-1906) to the discovery of piezoelectricity in materials such as tourmaline, quartz, boracite, sodium chlorate, Rochelle salt [Curie J. and Curie P. (1880), *C. R. Acad. Sci. Paris*, **91**, 294-295, *Développement, par pression, de l'électricité polaire dans les cristaux hémièdres à faces inclinées*]. The inverse piezoelectric effect was predicted by Lippmann G. [(1881), *Ann. Chim. Phy.* **24**, 145-178, *Principe de conservation de l'électricité*] and discovered by Curie J. and P. [(1881), *C. R. Acad. Sci. Paris*, **93**, 1137-1140, *Contractions et dilatations produites par des tensions électriques dans les cristaux hémièdres à faces inclinées*].

## See also

- An introduction to crystal physics (Teaching Pamphlet of the
*International Union of Crystallography*) - Section 3.2.2.6 of
*International Tables of Crystallography, Volume A*, 6^{th}edition - Section 1.1.4 of
*International Tables of Crystallography, Volume D*