COLLISION PROCESSES 

1. Types of Collision An electrical discharge is normally created from unionized gas by collision processes. These processes are mainly gas processes which occur due to the collision between the charged particles and gas atoms or molecules. These are of the following two types. Elastic collisions: Elastic collisions are collisions which when occur, no change takes place in the internal energy of the particles but only their kinetic energy gets redistributed. These collisions do not occur in practice. When electrons collide with gas molecules, a single electron traces' a zigzag path during its travel. But in between the collisions it is accelerated by the electric field. Since electrons are very light in weight, they transfer only a part of their kinetic energy to the much heavier ions or gas molecules with which they collide. These results in very little loss of energy by the electrons and therefore electrons gain very high energies and travel at a much higher speed than the ions. Therefore in all electrical discharges electrons play a leading role. Inelastic collisions: Inelastic collisions, on the other hand, are those in which internal changes in energy take place within an atom or a molecule at the expense of the total kinetic energy of the colliding particle. The collision often results in a change in the structure of the atom. Thus all collisions that occur in practice are inelastic collisions. For example ionization, attachment, excitation, recombination are inelastic collisions.
2. Mobility of Ions and Electrons When an ion moves through a gas under the influence of a static uniform electric field, it gains energy from the field between collisions and loses energy during collisions. Electric force on an electron/ion of charge e is eE, with the resulting acceleration being eE/m. When the energy gained by the ions from the electric field is small compared with the thermal energy, the drift velocity in the field direction W_{i} is proportional to the electrical field intensity E and may be expressed as follows: W_{i }= µ_{i }* E_{ }(1) Where µ_{i} is called the mobility of ions the mobility is mainly a characteristic of the gas through which the ion moves. At normal temperatures and pressures the mobility µ is of the order of several cm^{2}/voltsec. However, the concept of ionic mobility cannot be directly applied to electrons because of their extremely low mass. Any externally applied electric field will cause the electrons to gain energies much higher than their mean thermal energy. So the electron drift velocity, which has been defined as the average velocity, with which the centre of mass of the electron swarm moves in the direction of the field, is not a simple function of E/p, but is determined from the energy distribution function. From the kinetic theory the electron drift velocity We is given in microscopic terms as follows:
W_{e} = E_{e }/ 3ma^{2} d/dc (l c^{2}) (2) Where l is an equivalent mean free path of an electron with speed c
3. Diffusion Coefficient When particles possessing energy, which is exhibited as a random motion, are distributed unevenly throughout a space, then they tend to redistribute themselves uniformly throughout the space. This process is known as diffusion and the, rate at which this occurrence is governed by the diffusion passing through unit area in unit time perpendicular to the concentration gradient and for unit concentration gradient. In three dimensions this may be written as
Where n is the concentration of particles. Kinetic theory gives D in microscopic terms as follows D = 1/3 (lc) 4 Where l is the mean free path and c the random velocity, the average being taken over c In electrical discharges, whenever there is a nonuniform concentration of charges there will be migration of these charges from regions of higher concentration to regions of lower concentration. This process is called diffusion and this causes a deionising effect in the regions of lower concentration. The presence of walls confining a given volume increases the deionisation effect since charged particles lose their charge on hitting the wall. Both diffusion and mobility result in mass motion described by a drift velocity caused either by unbalanced collision forces (concentration gradient) or by the electric field itself. 4. Electron Energy Distributions For the development of a complete theory giving the relationship between the data concerning single collisions of electrons with gas molecules, and the experimentally obtained average properties of discharges, a knowledge of the electron energy distribution functions is essential. The most widely used distribution functions are the Maxwellian and Druyesteynian distributions which apply specifically to elastic conditions. The Maxwellian distribution has been found to apply where there is thermal equilibrium between the electrons and molecules. The distribution takes the form
Where C_{l} is the constant and is the mean energy. Druyesteynian distribution applies when the electron or ion energy is much greater than the thermal energy and is therefore expected to be more of application in transcends discharges. This distribution takes the form
Where C_{2} is another constant 5. Collision Cross Section Collision cross section is defined as the area of contact between two particles during a collision. In other words, the total area of impaCT'sThis area of contact is different for each type of collision. For example, the area of impact is more for ionisation while for an excitation it is less. For simultaneously, occurring processes such as ionization, excitation, charge transfer, chemical reactions, etc., the effective cross section is obtained by simple a addition of all the cross sections. If q, is the total cross section, and if q_{i},_{ }q_{e}, q_{c }..._{ }etc., are the cross sections for ionization, excitation, charge transfer, etc, respectively, then q_{t}= q_{i} +q_{e} + q_{c} + ……. Thus the use of collision cross sections instead of mean free paths has often proved to be advantageous. The collision cross section is also expressed in terms of the probability of a collision to take place, i.e., P = nq (7) which is the reciprocal of the mean free path. 6 The Mean Free Path (λ) The mean free path is defined as the average distance between collisions. When a discharge occurs large number of collisions occurs between the electrons and the gas molecules. Depending on the initial energy of the colliding electron, the distance between the two collisions vary The average of this is the mean free path. The free path is a random quantity and its mean value depends upon the concentration of particles or the density of the gas. The mean free path can be expressed as λ^{ =}k / p (8) Where k is a constant and p is the gas pressure in microns. The value of k for nitrogen is 5. From this equation it is seen that at a pressure of 1 torr, λ is 5 ^{x }10^{3 }cm. If the pressure is 10^{6} ton, then λ = 5 ^{x }10^{+3 }cm. From this it is seen that mean free path is very large at very low pressures and is very small at high pressures. 


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