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Quantitative analysis of gas circuit breaker physics through direct comparison of 3D simulations with experiment
N.P.Basse, M.Abrahamsson, M.Seeger and T.Votteler
2007 IEEE Pulsed Power andPlasma Science Conference
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Introduction
We study interruption of short-circuit current in high-voltage gas circuit breakers
Pressure produced by the arc is used to extinguish the arc, i.e. the self-blast principle
We measure the pressure buildup using two spatially separated sensors
The pressure and other measured quantities are compared to a 3D computational fluid dynamics (CFD) simulation
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CFD simulation setup
Left-hand plot shows the grid used for the CFD simulation A 180 degree cut is simulated
No turbulence is included
Right-hand plot shows the heating volume and the positions where pressure is simulated Position 3 is the
actual sensor location
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CFD pressure animation
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Current interruption phases
Sequence of events
1. Ablation controlled arc, backheating from arc zone to heating volume
2. Flow reversal when the heating volume pressure equals the arc pressure
3. Axially blown arc, flow from heating volume to arc zone
4. Arc extinction Plot above shows pressure
monitor points in the 3D simulation Here, we analyze results from
position 1 and 21
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Heating volume pressure and arc parameters
Left: Heating volume pressure
Right: Arc current and voltage
-0.02 -0.01 0 0.01 0.020
5
10
15
20
25
30
Time [s]
Pre
ssu
re [b
ar]
Measurement3D simulation
-0.02 -0.01 0 0.01 0.02-70
-35
0
35
70
Cu
rre
nt [
kA]
Time [s]-0.02 -0.01 0 0.01 0.02
-600
-300
0
300
600
Arc
vo
ltag
e [V
]
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Transient between flow reversal and CZ
A pressure transient a few ms before current zero (CZ) has been identified using cross correlation analysis
The oscillation is between the arc zone and the heating volume
Time [s]
Tim
ela
g [s
]
Cross correlation (hv1 and hv2)
-0.02 -0.01 0 0.01 0.02
-1.5
-1
-0.5
0
0.5
1
1.5
x 10-3
-1
-0.5
0
0.5
1
Time [s]
Tim
ela
g [s
]
Cross correlation (p1 and p21)
-0.02 -0.01 0 0.01 0.02
-1.5
-1
-0.5
0
0.5
1
1.5
x 10-3
-1
-0.5
0
0.5
1
Left simulations, right measurements
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Early transient in heating volume
Below we show auto correlation functions for both pressure measurements
An oscillation is observed at -0.01 s with a period of about 1.7 ms at one sensor position (left-hand plot)
Time [s]
Tim
ela
g [s
]
Auto correlation hv1
-0.02 -0.01 0 0.01 0.02
-1.5
-1
-0.5
0
0.5
1
1.5
x 10-3
-1
-0.5
0
0.5
1
Time [s]
Tim
ela
g [s
]
Auto correlation hv2
-0.02 -0.01 0 0.01 0.02
-1.5
-1
-0.5
0
0.5
1
1.5
x 10-3
-1
-0.5
0
0.5
1
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Pressure mixing
The pressure ratio 180 degrees apart is used to gauge the uniformity of pressure
Simulation (measurement) up to 1% (25%) difference, respectively
-0.02 -0.01 0 0.01 0.020.7
0.8
0.9
1
1.1
1.2
Time [s]
Pre
ssu
re r
atio
[hv2
/hv1
]
-0.02 -0.01 0 0.01 0.020.99
0.995
1
1.005
1.01
Time [s]
Pre
ssu
re r
atio
[p2
1/p
1]
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Temperature
Left: Temperature at sensor positions is very different after flow reversal Average heating volume temperature reflects current behavior
Right: With the sound speed of SF6 and dimensions of the circuit breaker, cross correlation periods can be used to derive average temperatures
-0.02 -0.01 0 0.01 0.020
500
1000
1500
2000
2500
Time [s]
Te
mp
era
ture
[K]
Averagep1p21
500 1000 1500 2000 2500 30000
200
400
600
800
1000
1200
Temperature [K]
SF
6 so
un
d s
pe
ed
[m/s
]
1 bar25 bar
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Pressure in arc zone and heating volume
Left: Simulated heating volume and arc zone pressure
Right: Cross correlation of the pressures
-0.02 -0.01 0 0.01 0.020
5
10
15
20
25
Time [s]
Pre
ssu
re [b
ar]
p1Stagnation point
Time [s]
Tim
ela
g [s
]
Cross correlation (p1 and psp
)
-0.02 -0.01 0 0.01 0.02
-1.5
-1
-0.5
0
0.5
1
1.5
x 10-3
-1
-0.5
0
0.5
1
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Pressure fluctuations
Power spectra of the two pressure measurements integrated up to 20 kHz are shown below
Most fluctuations during the final rise of the pressure
-0.02 -0.01 0 0.01 0.020
5
10
15
20
25
30
35
40
Time [s]
Pressure [bar]Fluctuations [a.u.]
-0.02 -0.01 0 0.01 0.020
5
10
15
20
25
30
35
40
Time [s]
Pressure [bar]Fluctuations [a.u.]