Dielectric Strength Definition
The dielectric strength is a property of a material which enables it to withstand electric stress without damage. It is usually expressed in terms of minimum electric stress (potential difference per unit distance) that will cause breakdown of dielectric under certain conditions of service.
The dielectric strength of an insulator or dielectric material is given by the maximum potential difference which a unit thickness of the material can withstand without breaking down. It is usually expressed in kV/mm.
For example, when we say that the dielectric strength of mica is 60 kV/mm, then it means that the maximum potential difference which one mm thickness of mica can withstand across it without breaking down is 60 kV or 60000 volts. If the potential difference exceeds this value, then mica insulation breaks down allowing a large current to pass through it.
The dielectric strength of various insulating materials is a very important factor in the design of high voltage electrical machines. It is usually adversely affected by moisture, contamination, elevated temperature, aging and mechanical stress.
It is also known as relative permittivity. We know that the capacitance of a capacitor depends upon the surface area of plates, the thickness of the dielectric and also on the nature of the material of the dielectric (i.e. dielectric constant).
From experiments, it is found that if the air is replaced by a dielectric of dielectric constant k in a capacitor, the value of capacitance is largely increased.
Dielectric Constant Definition
Dielectric constant is the ratio of the capacitance of a capacitor having a certain dielectric to the capacitance of the same capacitor with vacuum (or air) as the medium.
- Let there be a parallel plate capacitor of capacitance C, which has no dielectric material.
- and when we place a dielectric material between its plates, its capacitance becomes C’.
- then, the dielectric constant of the dielectric material will be C’/C.
Materials having a high value of dielectric constant are generally preferred for making capacitors of high capacity.
In most applications, the insulation consists of two or more insulating materials in series. The importance of dielectric constant lies in the fact that when an alternating voltage is applied to such a composite insulation, the voltage distribution across the insulation is found in inverse proportion to the dielectric constants of the materials involved.
For example, suppose there is an equal thickness of oil of dielectric constant 3 and paper of dielectric constant 4 in series. When a voltage is applied across it, 57% of voltage act across the oil and 43% across the paper.
Therefore, while designing a composite insulation care must be taken that the composite insulating materials have an appropriate dielectric constant in order that dangerously high voltage does not appear across any one of them.
When a perfect insulation is subjected to AC voltage, it is like applying AC voltage to a perfect capacitor. In such a case, the charging current will lead the applied voltage by 90o exactly and there will be no consumption of power. Only vacuum and purified gases approach this perfection.
Dielectric Loss Definition
In most insulating materials that is not the case. There is a definite amount of dissipation of energy when an insulator is subjected to AC voltage. This dissipated energy is known as the dielectric loss.
In commercial insulators, the leakage current (a current that flows to earth through the insulator) does not lead the applied voltage by exactly 90o. The phase angle is always less than 90o. The complementary angle δ = 90 – θ is known as dielectric loss angle.
For an insulator having a capacitance C and having a voltage V applied to it at a frequency f Hz, the dielectric power loss can be calculated as:
P = V22πfC tan δ watts
From the above equation, it is clear that power loss is dependent on tan δ so long as other factors are constant. Tan δ is known as power factor of the insulator.
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