Streamer Theory of Breakdown in Gases.pptx

Streamer Theory of Breakdown in Gases.pptx

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  CONDUCTION AND BREAKDOWN INGASES – STREAMER THEORY K. Karthikeyan, Associate Professor/EEE, Ramco Institute of Technology
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  TIME LAG FORBREAKDOWN  Actually, there is a time difference between the application of a voltage sufficient to cause breakdown and the occurrence of breakdown itself. This time difference is called the time lag.  The time t which lapses between the application of the voltage sufficient to cause breakdown and the appearance of the initiating electron is called a statistical time lag (ts) of the gap.  The appearance of electrons is usually statistically distributed. After the appearance of the electron, a time tt is required for the ionization processes to develop fully to cause the breakdown of the gap, and this time is called the formative time lag (tt).  The total time ts + tt = t is called the total time lag. 2
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  BREAKDOWN IN GASES– STREAMER THEORY  Townsend mechanism when applied to breakdown at atmospheric pressure was found to have certain drawbacks.  Current growth occurs as a result of ionization processes only. But in practice, breakdown voltages were found to depend on the gas pressure and the geometry of the gap.  The mechanism predicts time lags of the order of 10-5s, while in actual practice break-down was observed to occur at very short times of the order of 10-8s.  Townsend mechanism predicts a very diffused form of discharge, in actual practice, discharges were found to be filamentary and irregular. 3
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  BREAKDOWN IN GASES– STREAMER THEORY  Streamer theory postulated by Reather and Meak removes the limitations and drawbacks of Townsend’s theory.  According to the Townsend’s theory, electric spark discharge is due to the ionization of gas molecule by the collision of electron and release of electron from cathode due to positive ion bombardment.  But according to the streamer’s theory, it is not only ionization process responsible for breakdown of gas but such as formation of photon and space charge into the avalanche also are root cause of breakdown. 4
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  BREAKDOWN IN GASES– STREAMER THEORY  Reather explains the formation of spark due to streamer mechanism in which the secondary mechanism of photo ionization of gas molecule is involved.  This theory predict the development of a spark discharge directly from a single avalanche in which the space charge developed by the avalanche itself is said to transform the avalanche into a plasma streamer. 5
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  BREAKDOWN IN GASES– STREAMER THEORY 6 o A single electron starting at the cathode by ionization builds up an avalanche that crosses the gap. o The electrons in the avalanche move very fast compared with the positive ions. o By the time the electrons reach the anode the positive ions are in their original positions and form a positive space charge at the anode.
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  BREAKDOWN IN GASES– STREAMER THEORY 7
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  BREAKDOWN IN GASES– STREAMER THEORY  This enhances the field, and the secondary avalanches are formed from the few electrons produced due to photo-ionization in the space charge region.  This occurs first near the anode where the space charge is maximum and a further increase in the space charge.  This process is very fast and the positive space charge extends to the cathode very rapidly resulting in the formation of a streamer.  Comparatively narrow luminous tracks occurring at breakdown at pressures are called streamers. 8
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  BREAKDOWN IN GASES– STREAMER THEORY 9 Instantaneous recombination between positive ions and electrons releases photons which in turn generate secondary electrons by the photoionization process.
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  BREAKDOWN IN GASES– STREAMER THEORY  When the avalanche in the gap reaches a certain critical size the combined space charge field and externally applied field lead to intense ionization and excitation of the gas particles in front of the avalanche head.  These electrons under the influence of the electric field in the gap develop into secondary avalanches as shown in Fig.  Since photons travel with the velocity of light, the process leads to a rapid development of conduction channel across the gap. 10
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  STREAMER THEORY • Assoon as the streamer tip approaches the cathode, a cathode spot is formed and a stream of electrons rush from the cathode to neutralize the positive space charge in the streamer; the result is a spark, and the spark breakdown has occurred. 11
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  The three successivestages in the development of the streamer are shown diagrammatically in Fig. in which (a) shows the stage when avalanche has crossed the gap, (b) shows that the streamer has crossed half the gap length, and (c) shows that the gap has been bridged by a conducting channel. STREAMER THEORY 12
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  TOWNSEND’S VS STREAMER 13 Sl. No. Townsend’sTheory Streamer’s Theory 1. Theory states, current growth occurs as a result of ionization processes only. Theory states, breakdown voltages were bound to depend on gas pressure and geometry of the gap. 2. This mechanism predicts a very diffused form of discharge. This mechanism predicts discharges were found to be filamentary irregular. 3. Theory gives equation to prove Townsend’s criterion γ [exp (αd) – 1] = 1 Theory gives equation αd + ln (α/p) = 14.5 + ln (E/p) + 1/2 ln(d/p) this tells streamer’s criterion. 4. Primary and secondary ionization causes avalanche breakdown. The space charges fields play an important role in growth of avalanche in corona a spark discharges in non- uniform field gaps. 5. The mechanism predicts time lags of order of 10-5 sec. Breakdown occurs at very short times of the order of 10-8 sec. 6. Townsend’s mechanism operates for pd values below 1000 torr-cm and gas pressures varying from 0.01 to 350 torr. Streamer’s mechanism operates for higher values of pressure and higher value of pd.
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  PASCHEN'S LAW  Ithas been shown earlier that the breakdown criterion in gases is given as This equation shows a relationship between V and pd, and implies that the breakdown voltage varies as the product pd varies. 14
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  PASCHEN'S LAW • Thisequation is known as Paschen's law. • It is seen that the relationship between V and pd is not linear and has a minimum value for any gas. 15
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  BREAKDOWN IN NON-UNIFORMFIELDS AND CORONA DISCHARGES  If the electric field is uniform, a gradual increase in voltage across a gap produces a breakdown of the gap in the form of a spark without any preliminary discharges.  On the other hand, if the field is non-uniform, an increase in voltage will first cause a discharge in the gas to appear at points with highest electric field intensity, namely at sharp points or where the electrodes are curved or on transmission lines.  This form of discharge is called a corona discharge and can be observed as a bluish luminescence.  This phenomenon is always accompanied by a hissing noise, and the air surrounding the corona region becomes converted into ozone. 16
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  THANK YOU 17