Electrostriction

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In electromagnetism, electrostriction is a property of all electrical non-conductor or dielectrics. Electrostriction causes these materials to change their shape under the application of an electric field.[1]: 662  It is the dual property to magnetostriction.

Explanation

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Electrostriction is a property of all dielectric materials,[2] and is caused by displacement of ions (and the associated changes the electrons) in the crystal lattice upon being exposed to an external electric field. The cause of electrostrictive is linked to anharmonic effects.[2] Positive ions will be displaced in the direction of the field, while negative ions will be displaced in the opposite direction. This displacement will accumulate throughout the bulk material and result in an overall strain (elongation) in the direction of the field. The thickness will be reduced in the orthogonal directions characterized by Poisson's ratio. All insulating materials consisting of more than one type of atom will be ionic to some extent due to the difference of electronegativity of the atoms, and therefore exhibit electrostriction.[citation needed]

The resulting strain (ratio of deformation to the original dimension) is proportional to the square of the polarization. Reversal of the electric field does not reverse the direction of the deformation.[1]: 664 [2]

More formally, the electrostriction coefficient is a rank four tensor (Qijkl), relating the rank two strain tensor (εij) and the electric polarization density vector (i.e. rank one tensor; Pk)[2]

εij=QijklPkPl.

The electrostrictive tensor satisfies[1]: 666 

Qijkl=122εijPkPl.

The related piezoelectric effect occurs only in a particular class of dielectrics. Electrostriction applies to all crystal symmetries, while the piezoelectric effect only applies to the 20 piezoelectric point groups. Piezoelectricity is equivalent to the electrostrictive displacement of ions in ferroelectric materials.[2] Electrostriction is a quadratic effect, unlike piezoelectricity, which is a linear effect.[1]: 665 [2]

Materials

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Although all dielectrics exhibit some electrostriction, certain engineered ceramics, known as relaxor ferroelectrics, have extraordinarily high electrostrictive constants.[2] The most commonly used are

Magnitude of effect

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Electrostriction can produce a strain on the order of 0.1% for some materials.[1]: 662  This occurs at a field strength of 2 million volts per meter (2 MV/m) for the material PMN-15.[3] Electrostriction exists in all materials, but is generally negligible.[1]: 662 

Applications

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  • Sonar projectors for submarines and surface vessels
  • Actuators for small displacements [2]
  • Sensors, provided a bias electric field or pre-stress is present.[2]

See also

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References

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  1. ^ a b c d e f Lua error in Module:Citation/CS1/Configuration at line 2172: attempt to index field '?' (a nil value).
  2. ^ a b c d e f g h i Lua error in Module:Citation/CS1/Configuration at line 2172: attempt to index field '?' (a nil value).
  3. ^ Lua error in Module:Citation/CS1/Configuration at line 2172: attempt to index field '?' (a nil value).

Further reading

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