A dielectric is an insulator that can be electrodeled.The charged particles of the dielectric are tightly bound by the internal forces of atoms and molecules or the forces between molecules, so the charges of these particles are bound charges.Under the action of the external electric field, these charges can only move in the microscopic range, resulting in polarization.In the electrostatic field, there can be an electric field inside the dielectric, which is the basic difference between the dielectric and the conductor.
Dielectric includesGaseous, liquid and solid substances, including vacuum.Solid dielectricincludeCrystalline dielectricandAmorphous dielectricTwo major categories, the latter including glass, resin andPolymerWait, it's goodInsulating material。Everywhereelectric fieldGenerated under actionmacroscopicNot equal to zero onElectric dipole momentTherefore, the phenomenon of forming macroscopic bound charges is called electricitypolarizationThe materials that can produce the phenomenon of electrode are collectively called dielectrics.DielectricresistivityThey are generally very high and are calledinsulator。Some dielectricresistivityIt is not very high and cannot be calledinsulator, but because it can happenpolarizationProcess is also classified as dielectric.
change
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The positivenegative chargeOffset each other,macroscopicIt does not show electricity, but it is outsideelectric fieldThree types of changes can be generated under the action of:
② Molecules with original positive and negative centers coincident, outsideelectric fieldUnder the action, the positive and negative electric centers are separated from each other, which is calledDisplacement polarization;
③ Have inherentElectric dipole momentThe original orientation of the molecule is chaotic, and the total electric dipole moment on the macro scale is equal to zeroelectric fieldUnder the action ofElectric dipoleIt tends to be in a consistent arrangement, so that the macroscopic electric dipole moment is not equal to zero, which is called turningpolarization。
Applied to Displayedliquid crystalMaterials used in the application and protection of electrostatic effects, microwave dielectric materials used in stealth technology, and dielectric materials used as structural materials.
Special effects
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The theory and application of special effects of dielectrics constitute another aspect of dielectric physics[1]。These special effects include:
① Piezoelectric effect.When some crystals are deformed due to external forces, polarization will occur, and different sign bound charges will be formed on the opposite sides, which is called piezoelectric effect.There are many kinds of piezoelectric crystals, such as quartz, potassium sodium tartrate (Rochelle salt), potassium dihydrogen phosphate (KDP), ammonium dihydrogen phosphate (ADP), barium titanate, GaAs, zinc sulfide and other semiconductors and piezoelectric ceramics.The mechanical vibration of piezoelectric crystals can be converted into electrical vibration, which is often used to manufacture crystal oscillators. Its outstanding advantage is the high stability of the oscillation frequency. In radio technology, it can be used to stabilize the frequency of high-frequency oscillation. This kind of oscillator has been widely used in quartz clocks.Piezoelectric crystals are also widely used in electroacoustic devices such as microphones and electroacoustic heads.The piezoelectricity phenomenon can be used to measure the pressure, vibration and acceleration under various conditions[2]。
② Electrostriction.It is the inverse effect of piezoelectric effect.Some crystals will stretch or shorten under the action of electric field, which is called electrostriction.The electrostriction effect can be used to transform electrical vibration into mechanical vibration. Transducers commonly used to generate ultrasonic waves, earphones, tweeters, etc[2]。
③ Electret.The dielectric that can maintain polarization for a long time after removing external electric field or external mechanical action is called electret.Electret has both piezoelectric effect and thermoelectric effect.In technology, polar polymers are mostly used as electret materials.The electret can generate a strong electric field of 30 kV/cm.The ability of electret to store charge has been used in electrostatic photography and gas filters that absorb small particles in gas[2]。
④ Thermoelectric effect.Crystals with macroscopic electric dipole moment caused by spontaneous polarization and large thermal expansion coefficient are called thermoelectric crystals.The thermoelectric crystal in the state of spontaneous polarization has bound charges formed by polarization on the surfaces of the positive and negative ends of the electric dipole moment, but it does not show electrification due to the adsorption of different ions in the air.When the temperature changes, the volume of the thermoelectric crystal changes significantly, leading to a significant change in the polarization intensity, destroying the surface's electrical neutrality, and the excess charges adsorbed on the surface will be released. This phenomenon is called thermoelectric effect.Both artificially polarized ferroelectrics and electrets have thermoelectric effects.Thermoelectric effect has been used in infrared detection and thermal imaging technology[2]。
⑤ Electrothermal effect.As the reverse effect of thermoelectric effect, the dielectric (mostly electret) with electrothermal effect is called electrothermic.Under adiabatic conditions, when the permanent polarization strength of an electric heating body is changed by means of an external electric field, its temperature will change, which is called electrothermal effect.Adiabatic depolarization can reduce the temperature, and can be used to obtain ultra-low temperature as adiabatic demagnetization (see magnetocaloric effect).Common electrothermal materials include strontium titanate ceramics and polyvinylidene fluoride (PVF) electret[2]Body.
⑥ Electro optic effect.The effect of some isotropic transparent dielectrics becoming optical anisotropy under the action of electric field[2]。
⑦ Ferroelectricity.In some dielectric crystals, there are many small areas of spontaneous polarization. Each small area of spontaneous polarization is called a ferroelectric domain, and its linearity is on the order of micrometers.In the same ferroelectric domain, the orientation of each electric dipole moment is the same, and the spontaneous polarization direction of different ferroelectric domains is generally different, so the total electric dipole moment in the macro is zero.Under the external electric field, the polarization direction of each ferroelectric domain tends to be the same, and the polarization intensity P has a nonlinear relationship with the electric field intensity E.Under the repeated action of the alternating electric field with fixed peak value, the relationship curve between P and E is similar to the hysteresis loop (see ferromagnetism), which is called the hysteresis loop.The above properties are called ferroelectricity, and the dielectrics with ferroelectricity are called ferroelectrics.When the temperature rises to a certain critical value Tc, ferroelectric domains will be mutually resolved, ferroelectricity will disappear, and ferroelectrics will be transformed into ordinary paraelectric dielectrics. Tc is called ferroelectric Curie temperature.Ferroelectrics have high permittivity.Ferroelectrics must have both piezoelectricity and thermoelectricity[2]。
⑧ Ferroelasticity.Some crystals can form small areas of spontaneous strain in their interior, which are called ferroelastic domains. The direction (domain state) of spontaneous strain in the same ferroelastic domain is the same, and the domain states of any two ferroelastic domains are the same or mirror symmetric.The applied stress can make the ferroelastic domain transition from one domain state to another.When the external stress changes, the strain lags behind the stress change, and the relationship between stress and strain is nonlinear.Under the action of periodic external stress, the relationship curve between strain and stress is similar to the hysteresis loop, which is called the force hysteresis loop.The above properties are called ferroelasticity, and the dielectrics with ferroelasticity are called ferroelastic bodies.The permittivity, refractive index, conductivity, thermal expansion coefficient, thermal conductivity, elastic modulus and electrostriction rate of the ferroelastic body vary with the direction, and this directivity will change with the stress. Using these characteristics has broad application prospects in manufacturing force sensitive devices[1-2]。
classification
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1. Equivalent positive center and equivalent negative center of molecule:
All dielectrics are composed of molecules and atoms. The electric effect of all positive charges in each molecule on the outside can be equivalent to the effect of the equivalent point charge concentrated at a certain point. The position of the equivalent point charge is called the positive center of the molecule;Similarly, the electrical effect of all negative charges in each molecule on the outside can be equivalent to the effect of the equivalent point charge concentrated at a certain point, and the position of the equivalent point charge is called the negative point center of the molecule;
2. Polar molecule dielectric:
Dielectric in which the equivalent positive center of each molecule does not coincide with the equivalent negative center;The positive center and negative center can be replaced by the same amount of different sign charge respectively, and there is a relative displacement between them, so that the electrical effect of each molecule on the outside can be equivalent to the effect of an electric dipole.
3. Electrodeless molecular dielectrics:
A dielectric in which the equivalent positive center of each molecule coincides with the equivalent negative center.
It can be considered that the positive charge q of each molecule is concentrated at a point, which is called the "center of gravity" of the positive charge, and the negative charge - q is concentrated at a point, which is called the "center of gravity" of the positive and negative charges;Define the vector path from the center of gravity of the negative charge to the center of gravity of the positive charge as, then the molecule can form an electric dipole[3]。
Electrical structure
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(1) The electron is tightly bound by the nucleus;
(2) In the electrostatic field, the positive and negative charges in the dielectric neutral molecules only produce microscopic relative motion;
(3) When the electrostatic field interacts with the dielectric, the dielectric molecule is simplified as an electric dipole.The dielectric consists of a large number of tiny electric dipoles;
(4) Dielectric in external electric field → polarization → polarization charge → additional electric field → acting on dielectric → achieving electrostatic balance[3-4]。
difference
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In electricians, it is generally believed that materials with resistivity exceeding 10 Ω/cm are classified as dielectrics.The charged particles of the dielectric are tightly bound by the internal forces of atoms and molecules or the forces between molecules, so the charges of these particles are bound charges.Under the action of external electric field, these charges can only move in the microscopic range to producepolarization。stayelectrostatic fieldThe electric field can exist in the dielectric, which is the basic difference between dielectric and conductor.
The phenomenon that the vector sum of the electric dipole moment in the dielectric is not zero.Dielectric can be divided into two categories: one is right and wrongPolarityDielectricnegative chargeThe other is polar dielectrics (under normal conditions, the average positions of positive and negative charges of molecules in the medium do not coincide).Withoutelectric fieldEquivalent of non-polar dielectric molecules when actingElectric dipole momentIs zero;Due to the disordered arrangement of polar dielectric molecules, the vector sum of their equivalent electric dipole moments is also zero.Outsideelectric fieldWhen acting, the positive of non-polar dielectric moleculenegative chargeAverage position relative displacementElectric dipole momentSteering occurs.In this waypolarizationPhenomenon.polarizationDegree of, availableElectric polarization intensityP means.P is the electric dipole moment per unit volume, that is, it is a vector whose unit isInternational System of UnitsThe middle is coulomb/m2.According to experiments, many dielectricElectric polarization intensityP andelectric field intensityE is proportional, i.e
Or expressed as the constitutive equation D of the dielectric=εIn formula EεIs the dielectric constant of the dielectric.according toGaussianFlux theorem
dielectric
This shows thatElectric displacementThe flux of D is determined byFree chargeQf.Although the bound charge may affect the distribution of D, it will not emit the flux of D.In some cases, it is more convenient to use this formula, because this formulaEqual signThe right term does not contain bound charges.stayTime-varying electromagnetic fieldThe time change rate of electric displacement isDisplacement currentDensity.The unit of electric displacement isInternational System of UnitsWhere is coulomb/m2 (C/m2).
application
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stayElectrotechnicsMedium, dielectric is mainly used as electricalinsulationMaterials, so dielectrics are also called electrical insulating materials.With the development of science and technology, it is found that some dielectrics havePolarization processRelevant special performance.If notSymmetrical centerThe crystal dielectric ofpolarization, i.ePiezoelectricity;There is no symmetry center, but there is a unique polar crystal with different directionsSpontaneous polarizationWhen temperature change can cause polarizationPyroelectricSex;When the spontaneous polarization dipole moment energy is appliedelectric fieldIts polarization intensity is related to the applied electric fieldcurveAndFerromagnetic materialOfMagnetizationAndmagnetic fieldThe relationship curve of is very similar, that is, it hashysteresis loop (Ferroelectricity)。havePiezoelectricity、Pyroelectricity、FerroelectricityAre called piezoelectric materialsPyroelectric materialFerroelectric materials.These materials with special properties are collectively referred to as functional materials.It is an important part of the dielectric.It can be used for conversion between machinery, heat, sound, light and electricity, and has extremely important applications in national defense, detection, communication and other fields.