What (who) is Dielectric complex reluctance - definition
Dielectric complex reluctance
Dielectric complex reluctance is a scalar measurement of a passive dielectric circuit (or element within that circuit) dependent on sinusoidal voltage and sinusoidal electric induction flux, and this is determined by deriving the ratio of their complex effective amplitudes. The units of dielectric complex reluctance are F^{-1} (inverse Farads - see Daraf) [Ref.
Dielectric
ELECTRICALLY POORLY CONDUCTING OR NON-CONDUCTING, NON-METALLIC SUBSTANCE OF WHICH CHARGE CARRIERS ARE GENERALLY NOT FREE TO MOVE
Dielectric level; Paraelectricity; Dielectric dispersion; Dipolar polarization; Ionic polarization; Dielectric media; Dielectric medium; Dielectric relaxation; Debye relaxation; Debye equation; Dielectrics; Dialectric; Dielectric materials; Relaxation time of electrons; Dielectric relaxation as a chemical rate process; Dielectric relaxation asa chemical rate process; Paraelectric; Dielectric polarization; Dielectric properties; Dielectric response; Perfect dielectric; Dielectric material; Paraelectrics; Ionic polarisation
·noun Any substance or medium that transmits the electric force by a process different from conduction, as in the phenomena of induction; a nonconductor. separating a body electrified by induction, from the electrifying body.
Dielectric Polarization
ELECTRICALLY POORLY CONDUCTING OR NON-CONDUCTING, NON-METALLIC SUBSTANCE OF WHICH CHARGE CARRIERS ARE GENERALLY NOT FREE TO MOVE
Dielectric level; Paraelectricity; Dielectric dispersion; Dipolar polarization; Ionic polarization; Dielectric media; Dielectric medium; Dielectric relaxation; Debye relaxation; Debye equation; Dielectrics; Dialectric; Dielectric materials; Relaxation time of electrons; Dielectric relaxation as a chemical rate process; Dielectric relaxation asa chemical rate process; Paraelectric; Dielectric polarization; Dielectric properties; Dielectric response; Perfect dielectric; Dielectric material; Paraelectrics; Ionic polarisation
A term due to Faraday. It expresses what he conceived to be the
condition of a dielectric when its opposite faces are oppositely
electrified. The molecules are supposed to be arranged by the
electrification in a series of polar chains, possibly being originally
in themselves seats of opposite polarities, or having such imparted to
them by the electricities. The action is analogous to that of a magnet
pole on a mass of soft iron, or on a pile of iron filings.
