Alexander Fufaev

Formula: Polarization of a Material

External field is weakened in the dielectric material

Polarization

Unit
Polarization describes the density of electric dipoles in a material (number per volume) and induces a polarization field \( \class{purple}{E_{\text{p}}} \), which can be aligned either opposite or in the same direction as the external electric field, thereby amplifying or weakening the external electric field.

Electric field (E field)

Unit
External electric field in which the dielectric material is situated.

Electric susceptibility

Unit
Electric susceptibility indicates how well a material can be polarized by an external electric field \( \class{purple}{E} \). In other words, it quantifies how effectively the external electric field is weakened or strengthened within the material.
  • For \( \class{green}{\chi_{\text{e}}} > 0 \), the external electric field is amplified within the material.
  • For \( \class{green}{\chi_{\text{e}}} < 0 \), the external electric field is weakened within the material.
  • For \( \class{green}{\chi_{\text{e}}} = 0 \), it is neither weakened nor strengthened. The "material" is vacuum.
Material Electric susceptibility
Vacuum 0
Air (0°C) 0.0005
Glass 4 bis 9
Water (0°C) 87
Water (40°C) 72.4
Ice (-20°C) 15
Hydrogen Cyanide 94
Ethanol (20°C) 24.8
Electric susceptibility of some materials