Ferroelectricity

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Ferroelectricity is a characteristic property of certain materials that exhibit a spontaneous electric polarization that can be reversed by the application of an external electric field. This phenomenon is closely related to ferromagnetism, in which a material exhibits a permanent magnetic moment. The term "ferroelectric" was coined by analogy to ferromagnetism, though the two phenomena are not related to iron, nor do they have similar mechanisms.

Overview[edit | edit source]

Ferroelectric materials are a subclass of piezoelectric materials, which can generate an electric charge in response to applied mechanical stress. However, not all piezoelectric materials are ferroelectric. Ferroelectricity is observed in materials that possess a non-centrosymmetric crystal structure, allowing for a permanent electric dipole moment in the absence of an electric field. When an external electric field is applied, the direction of the dipole moment can be switched, making these materials useful in a variety of applications, including memory devices, actuators, and sensors.

History[edit | edit source]

The discovery of ferroelectricity dates back to the early 20th century, with the first observation in Rochelle salt by Valasek in 1920. Since then, a wide range of materials have been found to exhibit ferroelectric properties, including barium titanate (BaTiO3) and lead zirconate titanate (PZT), which are among the most widely used ferroelectric materials today.

Mechanism[edit | edit source]

The ferroelectric behavior is primarily due to the displacement of ions within the material's crystal lattice, leading to the formation of a spontaneous polarization. This displacement is often related to the material's specific crystal structure, which lacks a center of symmetry. In the paraelectric phase (above the Curie temperature), the material does not exhibit spontaneous polarization due to thermal agitation. However, below the Curie temperature, the material undergoes a phase transition to a ferroelectric phase, where the crystal structure allows for a spontaneous polarization to occur.

Applications[edit | edit source]

Ferroelectric materials have a wide range of applications due to their unique properties. They are used in:

  • Non-volatile memory devices, such as ferroelectric random-access memory (FeRAM), which utilize the ability of ferroelectric materials to retain their polarization state without power.
  • Piezoelectric sensors and actuators, which exploit the piezoelectric effect in ferroelectric materials for converting mechanical stress into electrical signals, and vice versa.
  • Optical devices, including modulators and switches, which leverage the electro-optic effect in ferroelectric materials to control light propagation.

Challenges and Future Directions[edit | edit source]

While ferroelectric materials offer significant advantages, there are challenges in their application, including fatigue, aging, and scalability for high-density memory devices. Research is ongoing to develop new ferroelectric materials with improved properties, such as higher Curie temperatures, reduced coercive fields, and enhanced endurance. Additionally, the exploration of thin-film ferroelectrics and nanostructured ferroelectrics holds promise for the next generation of electronic and optical devices.

See Also[edit | edit source]


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Contributors: Prab R. Tumpati, MD