Electrical Insulating Materials (or Dielectrics) are materials in which electrostatic - PowerPoint Presentation

1. Electrical Insulating Materials (or Dielectrics) are materials in which electrostatic fields can remain almost indefinitely. These materials thus offer a very high resistance to the passage of direct currents. However, they cannot withstand an infinitely high voltage. When the applied voltage across the dielectric exceeds a critical value the insulation will be damaged. The dielectrics may be gaseous, liquid or solid in form. Breakdown in Gaseous InsulationGaseous dielectrics in practice are not free of electrically charged particles, including free electrons. The electrons, which may be caused by irradiation or field emission, can lead to a breakdown process to be initiated. These free electrons, however produced, on the application of an electric field are accelerated from the cathode to the anode by the electric stress applying a force on them. They acquire a kinetic energy (½ mxuxu ) as they move through the field.

2. The energy is usually expressed as a voltage (in electron volt, eV, where e is the charge on an electron) as the energies involved are extremely small. [The energy Ei = e Vi is expressed in electron volt. 1 e V = 1.6 x 10-19 J]. These free electrons, moving towards the anode collide with the gas molecules present between the electrodes. In these collisions, part of the kinetic energy of the electrons is lost and part is transmitted to the neutral molecule. If this molecule gains sufficient energy (more than the energy Ei necessary for ionization to occur), it may ionize by collision. The (mean) number of ionizing collisions by one electron per unit drift across the gap is not a constant but subject to statistical fluctuations. The newly liberated electron and the impinging electron are then accelerated in the field and an electron avalanche is set up. Further increase in voltage results in additional ionizing processes. Ionization increases rapidly with voltage once these secondary processes take place, until ultimately breakdown occurs. It is worth noting that in uniform fields, the ionization present at voltages below breakdown is normally too small to affect engineering applications. In non-uniform fields, however, considerable ionization may be present in the region of high stress, at voltages well below breakdown, constituting the well known corona discharge.

3. Ionisation processes in gas dischargesThe electrical breakdown of a gas is brought about by various processes of ionisation. These are gas processes involving the collision of electrons, ions and photons with gas molecules, and electrode processes which take place at or near the electrode surface [Electrons can be emitted from the cathode if the stress is around 100 - 1000 kV/cm due to field emission]. Ionisation is the process by which an electron is removed from an atom, leaving the atom with a net positive charge (positive ion). Since an electron in the outermost orbit is subject to the least attractive force from the nucleus, it is the easiest removed by any of the collision processes. The energy required to remove an outer electron completely from its normal state in the atom to a distance well beyond the nucleus is called the first ionisation potential. The reciprocal process of an electron falling from a great distance to the lowest unoccupied orbit is also possible. In this case, a photon will be emitted having the same energy as previously absorbed. The processes that are primarily responsible for the breakdown of a gas are ionization by collision, photo-ionization, and the secondary ionization processes. In insulating gases (also called electron-attaching gases) the process of attachment also plays an important role.

4. Primary Ionization: (a) Ionization by Collision

5. (b) Photoionization

6. Secondary Ionization Processes Secondary ionisation processes by which secondary electrons are produced are the one which sustain a discharge after it is established due to ionisation by collision and photo-ionization. They are briefly described below. (a) Electron Emission due to Positive Ion Impact Positive ions are formed due to ionisation by collision or by photo-ionisation, and being positively charged, they travel towards the cathode. A positive ion approaching a metallic cathode can cause emission of electrons from the cathode by giving up its kinetic energy on impact. If the total energy of the positive ion, namely, the sum of its kinetic energy and the ionisation energy, is greater than twice the work function of the metal, then one electron will be ejected and a second electron will neutralise the ion. The probability of this process is measured as ϒi which is called the Townsend's secondary ionisation coefficient due to positive ions and is defined as the net yield of electrons per incident positive ion. ϒi increases with ion velocity and depends on the kind of gas and electrode material used

7. (b) Electron Emission due to Metastable and Neutral Atoms A metastable atom or molecule is an excited particle whose lifetime is very large (1/1000 s) compared to the lifetime of an ordinary particle (1/100000000 s). Electrons can be ejected from the metal surface by the impact of excited (metastable) atoms, provided that their total energy is sufficient to overcome the work function. This process is most easily observed with metastable atoms, because the lifetime of other excited states is too short for them to reach the cathode and cause electron emission, unless they originate very near to the cathode surface. Electron Attachment Process The types of collisions in which electrons may become attached to atoms or molecules to form negative ions are called attachment collisions. Electron attachment process depends on the energy of the electron and the nature of the gas and is a very important process from the engineering point of view. All electrically insulating gases, such as Oxygen, CO2, Cl2, F2, SF6 etc exhibit this property. An electron attachment process can be represented as: Atom + electron + k ---> negative atomic ion + (Ea + K) The energy liberated as a result of this process is the kinetic energy K plus the electron affinity Ea. In the attaching or insulating gases, the atoms or molecules have vacancies in their outermost shells and, therefore, have an affinity for electrons. The attachment process plays a very important role in the removal of free electrons from an ionised gas when arc interruption occurs in gas-insulated switchgear

8. Breakdown Characteristics in Gases-->Two mechanisms of breakdown in gases is known. These are Townsend breakdown and Streamer breakdown mechanism.Electron Avalanche Mechanism (Townsend Breakdown Process) One of the processes which are considered in breakdown is the Townsend breakdown mechanism. It is based on the generation of successive secondary avalanches to produce breakdown. Suppose a free electron exists (caused by some external effect such as radio-activity or cosmic radiation) in a gas where an electric field exists. If the field strength is sufficiently high, then it is likely to ionize a gas molecule by simple collision resulting in 2 free electrons and a positive ion. These 2 electrons will be able to cause further ionization by collision leading in general to 4 electrons and 3 positive ions. The process is cumulative, and the number of free electrons will go on increasing as they continue to move under the action of the electric field. The swarm of electrons and positive ions produced in this way is called an electron avalanche. In the space of a few millimetres, it may grow until it contains many millions of electrons.This is shown in the following figure.

9.

10. Townsend’s current growth equation

11. Current growth in the presence of secondary processes

12.  Townsend’s criteria for breakdown