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Paraelectricidad

De Wikipedia, la enciclopedia libre

La paraelectricidad se refiere a la propiedad que presentan numerosos materiales a polarizarse cuando son sometidos a la influencia de un campo eléctrico. A diferencia de la ferroelectricidad, este fenómeno se produce incluso cuando no existen dipolos permanentes presentes en el material.[1]​ Dado que no existe alineación residual de dipolos, al cesar la influencia del campo eléctrico, la polarización se desvanece.[2]​ Los materiales que presentan esta propiedad, se conocen como materiales paraeléctricos.

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Transcription

Véase también

Referencias

  1. ↑ Chiang, Y. et al: Physical Ceramics, John Wiley & Sons 1997, New York
  2. ↑ Arthur Kip: Fundamentos de Electricidad y Magnetismo, McGraw-Hill, México, 1988
Esta página se editó por última vez el 26 ago 2020 a las 15:30.
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