4. What is the difference between dielectric
and insulator?
The material which stores the electrical energy in an
electric field is known as the dielectric material,
whereas the material which blocks the flow of
electrons is known as the insulators.
5. PROPERTIES OF DIELECTRICS
Insulating ability
- Dielectrics prevent the flow of electric current and are valued for their high electrical
resistance.
Polarization
- Dielectrics can be polarized by an applied electric field, leading to the alignment of charges
within the material.
Permittivity and susceptibility
- Permittivity refers to a material's ability to permit the electric field, while susceptibility
measures the degree of polarization.
6. Types of Dielectrics
Linear vs. non-linear dielectrics
- Linear dielectrics exhibit a proportional response to the applied electric field,
while non-linear dielectrics show a more complex relationship.
Homogeneous vs. heterogeneous dielectrics
- Homogeneous dielectrics have uniform properties throughout, whereas
heterogeneous dielectrics have variations in composition.
8. POLAR DIELECTRICS
Assymetric arrangement of atoms, which means centers of gravity
of positive and negative charges don’t coincide, even in absence of
external field.
Polar dielectrics are polar compounds that do not conduct
electricity.
Ex. Ammonia, and HCI
9. NONPOLAR DIELECTRICS
Symmetric arrangement of atoms, which means centers of gravity
of positive and negative charges coincide in absence of external
electric field.
Nonpolar dielectrics are nonpolar compounds that cannot conduct
electricity.
Ex. Benzene, methane, carbon dioxide
10.
11. POLARIZATION
When a dielectric material is placed in an electric field, the
positive and negative charges within the atoms or
molecules are separated, creating an electric dipole
moment. This phenomenon is known as polarization.
12. Polarization Mechanisms
Orientation polarization
- Polarization due to the alignment of molecules with an external electric field.
Electronic polarization
- Polarization caused by the displacement of electrons within atoms or
molecules.
Ionic polarization
- Polarization resulting from the movement of ions in response to an electric
field.
13. ELETRONIC POLARIZATION
In atoms or molecules, electrons can be displaced
from their equilibrium positions, creating an induced
dipole moment.
14. DIELECTRIC IN AN ELECTRIC FIELD
Dipole moment: p = q x d
Note that p, the electric
dipole moment, is a vector: it
has direction.
Where q is the (absolute
value of the) charge of
electron cloud that was
displaced.
15. IONIC POLARIZATION
Ionic polarization occurs in ionic compounds, in which the
oppositely charged ions move in opposite directions under the
influence of the electric field to produce a net dipole moment in
them.
This type of polarization typically occurs in ionic crystal elements
such as NaCl, KCl, and LiBr.
16. IONIC POLARIZATION
To undergo ionic polarization, a material must
have an ionic structure, it must be composed of
cations and anions.
This ion pair already possesses a dipole moment
before the application of the electric field.
17. The applied field causes the bond to
stretch.
IONIC POLARIZATION
Reverse field: this field causes compression of
the bond and thus decrease the dipole
moment.
18. ORIENTATIONAL POLARIZATION
Oriental polarization occurs in polar substannces. These substamce
exhibit dipole moment even in the absence of external electric field.
When such materials are subjected to an external electric field, the
permanent molecular dipoles rotate about their axis of symmetry to
align with the applied field.
Ex: H2O in its liquid form
19. ORIENTAL POLARIZATION
Some molecules possess a permanent dipole there is always a separation of charge within the
molecule, even in the absence of an electric field. The example shown here is H2O.
20. ORIENTAL POLARIZATION
Consider a material containing many such
dipoles. In naturally non- polar materials
like water, the dipoles are randomly
arranged as a result of thermal motion.
Therefore the dipole moments from
different molecules cancel out and the net
polarization is zero.
21. ORIENTAL POLARIZATION
The dipoles rotate in order to align with
the electric field. As a result, they also
align with each other. Dipole moments
no longer cancel out, and the material
develops a net polarization.
22. SPACE CHARGE POLARIZATION
The space charge, or interfacial polarization, is produced by the separation of mobile positively
and negatively charged particles under an applied field, which form positive and negative space
charges in the bulk of the material or at the interfaces between different materials.
23. Dielectrics in Capacitors
A capacitor is a device used for storing charge. It normally consists of two conducting plates
with a dielectric material between them, although an “empty capacitor” – one with a vacuum
between the plates – may also be used in some applications.
Capacitors consist of two conductive plates separated by a dielectric, storing energy in an
electric field.
24. DIELECTRIC CONSTANT
The dielectric constant of a material provides a measure of its effect on a
capacitor. It is the ratio of the capacitance of a capacitor containing the dielectric
to that of an identical but empty capacitor.
Permittivity is a quantity that describes the effect of a material on an electric
field: the higher the permittivity, the more the material tends to reduce any field
set up in it.
25. Dielectric Strength
Dielectric strength is the ability of a material to withstand electric
stress without undergoing breakdown.
Factors affecting dielectric strength
- Factors include material purity, temperature, and thickness.
26. DIELECTRIC LOSS
Dielectric loss is the dissipation of energy through the movement of charges in
an alternating electromagnetic field as polarization switches direction.
27. Dielectric Breakdown
Dielectric breakdown is the sudden failure of a dielectric material, leading to
the loss of its insulating properties.
Factors influencing breakdown strength
- Factors include material composition, temperature, and applied electric field
strength.
28. APPLICATION OF DIELECTRICS
A major use of dielectrics is in fabricating capacitors. These have
many uses including storage of energy in the electric field between
the plates, filtering out noise from signals as part of a resonant
circuit, and supplying a burst of power to another component.
29. SUMMARY
Dielectrics are electrical insulators that support charge.
The properties of dielectrics are due to polarization.
There are three main mechanisms by which polarization arises on the microscopic scale: electronic (distortion of
the electron cloud in an atom), ionic (movement of ions) and orientational (rotation of permanent dipoles).
A capacitor is a device that stores charge, usually with the aid of a dielectric material. Its capacitance is defined
by Q = C V
The dielectric constant κ indicates the ability of the dielectric to polarize. It can be defined as the ratio of the
dielectric’s permittivity to the permittivity of a vacuum.
The dielectric constant is also affected by structure, as this affects the ability of the material to polarize.
Polar dielectrics show a decrease in the dielectric constant as temperature increases.
Dielectric loss is the absorption of energy by movement of charges in an alternating field, and is particularly high
around the relaxation and resonance frequencies of the polarization mechanisms.
Sufficiently high electric fields can cause a material to undergo dielectric breakdown and become conducting.
Diaelectric material are essential in the technologies we use everyday. For, example they are use for energy storage in capacitors and to enhance devices based on semiconductors.they are also present in liquid crystal displays.
Lets look at the word itself dielectric, the word is contructed from the greek word dia which means passing trhough. And electric refers to electric field, GIVING YOU DIAELECTRIC, this term was proposed by a scientist and philosopher from the 19th century. Diaelectric is difficult to spell, so with time, it compressed into the word dielectrc.
Dielectrics are materials that don't allow current to flow. They are more often called insulators because they are the exact opposite of conductors. But usually when people call insulators “dielectrics,” it's because they want to draw attention to a special property shared by all insulators: polarizability.
So basically, dielectric material is a storage for electrical energy, while insulator are known to block electrons
, which means centers of gravity of positive and negative charges don’t coincide, even in absence of external field.
As you can see the polar is scattered or assymetric while the nonpolar is symmetric with eac other. Now lets move on to the types of polarization. Now what is polarization?
There are three main polarisation mechanisms that can occur within a dielectric material: electronic polarisation, ionic polarisation (sometimes referred to as atomic polarisation) and orientational polarisation.
Here is an example of electronic polarization
Lets expose a dielectric material to the electrical field, as you can see in the picture , applying electric field, the positive and negative charges dissociate and moved away from each other creating a dipole. If the center of charges end uo at a distance d from each orher,we say that this atom has an electric dipole moment , once the charge displacement has taken place, the material becomes polarized. Polarized material induces dipole moments.
IF a material contains ions,
lonic polarization occur due to the displacement of cation and anion in opposite directions with the application of electric field in the ionic solids.
Cation are ions that are positively charge and anions are ions are negatively charged
This is observed in the materials that posses symmetric molecules.
It does not occur in typical covalent crystals such as diamond.
lonic polarization is independent of temperature.
Cation are ions that are positively charge and anions are ions are negatively charged
And that is ionic polarization, next is the oriental polarization
It is due to the presence of polar molecules in the dielectric material which have permanent dipole moment.
When electric field is applied on the dielectric material, it tries to align the dipole in its direction that results in the existence of dipole moment in the material.
It occurs in asymmetric molecules.
Its depends on the temperature.
Note that such permanent dipoles may also exist within ionic structures, e.g. crystals in which the cations are off-centred within the unit cells and do not coincide with the centre of negative charge.
ALL non-conducting materials are capable of electronic polarisation, which is why all insulators are dielectric to some degree. In contrast, the ionic and orientational modes are only available to materials possessing ions and permanent dipoles respectively. Another contribution to polarization is space charge, or the accumulation of mobile charges at structural surfaces and interfaces. Rather than being a direct property of a material this is only a feature of heterostructures, and hence is not discussed further here.
ALL non-conducting materials are capable of electronic polarisation, which is why all insulators are dielectric to some degree. In contrast, the ionic and orientational modes are only available to materials possessing ions and permanent dipoles respectively
space charge, or the accumulation of mobile charges at structural surfaces and interfaces. Rather than being a direct property of a material this is only a feature of heterostructures, and hence is not discussed further here.
Each capacitor has a capacitance
The capacitance is affected by various factors, such as the capacitor geometry, however here we shall only deal with the effect of the dielectric material chosen to occupy the space between the plates.
An alternative definition of the dielectric constant relates to the permittivity of the material.
Since the dielectric material reduces the field by becoming polarised, an entirely equivalent definition is that the permittivity expresses the ability of a material to polarise in response to an applied field.
The dielectric constant (sometimes called the ‘relative permittivity’) is the ratio of the permittivity of the dielectric to the permittivity of a vacuum, so the greater the polarisation developed by a material in an applied field of given strength, the greater the dielectric constant will be.
If we have dielectric strength of course we also have dielectric loss
AN efficient dielectric supports a varying charge with minimal dissipation of energy in the form of heat. There are two main forms of loss that may dissipate energy within a dielectric. In conduction loss, a flow of charge through the material causes energy dissipation.
Dielectric loss is especially high around the relaxation or resonance frequencies of the polarisation mechanisms as the polarisation lags behind the applied field, causing an interaction between the field and the dielectric’s polarisation that results in heating.
ielectric loss tends to be higher in materials with higher dielectric constants
At high electric fields, a material that is normally an electrical insulator may begin to conduct electricity – i.e. it ceases to act as a dielectric. This phenomenon is known as dielectric breakdown
The larger the dielectric constant, the more charge the capacitor can store in a given field