Paschen’s law
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Transcript of Paschen’s law
Paschen’s Law
Sustained Townsend discharge leads to spark then arc (flashover). Formulated mathematically by Paschen, (see p 52)
The flashover voltage is a function of the product of the gas pressure and the gap length for an uniform field
Implications in practice:
- Altitude effect
- Compressed gases
- Vacuum contactors
Approximation for curve:
0.1
1
10
100
1000
10000
0.001 0.01 0.1 1 10 100
pressure x gap length (cm bar) B
reakd
ow
n V
olt
ag
e (
kV
)
Empirical Formula (Eq. 3.11)
Paschen Equation ( Eq. 3.10)
pdpdVc
36.2472.6
a) Low pressure(few collisions:low ionization)
b) High pressure(low kinetic energy:low ionization)
c) Medium pressure( optimal: highionization)
+ - + - + -
Paschen’s Law
Low gas density - more kinetic energy gained but less collisions High gas density – more collisions but less energy gained
Streamer discharges
A self-sustaining discharge can develop from a single avalanche
Space charge (ions) distort and enhance field
Photons cause further avalanches in high field regions
Streamer discharges occur if n 5 .108
Occurs for non-uniform long gaps and at high pressures
GASES – FLASHOVER - STREAMER MECHANISM –
MEDIUM GAPS (> 5 Bar.mm)
Cath
ode (
-)
Ano
de (
+)
E - Field
Photons
Avalanche with x = 20
Asymmetrical, non uniform gaps:
The polarity Effect
_ +
_+
Region of high field strength near the sharp point, in both cases
Avalanches are formed in these regions, leaving a positive space charge in this region.
In the case of the positive tip the space charge has the same polarity as the electrode and assists in increaing the field.
In the case of the negative tip the space charge opposes the polarity of the tip.
A lower flashover voltage is thus obtained for the positive tip, compared to the negative one.