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An experimental investigation on the mechanisms of the electrictriggerpulsegenerated bubble in a tri

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2- Water is used as the dielectric in water gap switches for pulsed ... and also from Professor G Woolsey for his advice and assistance during this research. ... – PowerPoint PPT presentation

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Title: An experimental investigation on the mechanisms of the electrictriggerpulsegenerated bubble in a tri


1
An investigation into the breakdown
mechanisms of a triggered water gap
switch     Mohsen Saniei     Institute for
Energy and Environment University of
Strathclyde Glasgow G1 1XW
2
Introduction
  • 1- Water has
  • a- High dielectric constant (?81)
  • b- High dielectric strength (1MV/cm)
  • c- High energy storage density

2- Water is used as the dielectric in water gap
switches for pulsed power applications
3
Aims and objectives
1-Investigating the effect of triggering on the
breakdown of a water gap 2- Investigating the
breakdown mechanism in triggered water gaps
4
Electric set-up Schematic
  • Main voltage is generated by the discharge of the
    80nF high voltage capacitor by activating the
    trigatron switch
  • Trigger pulse for the water gap is generated by a
    4X Blumlein generator

5
Triggering effect on the time lag to breakdown
Triggering decreases the time lag to breakdown
6
Triggering effect on water gap breakdown
Triggering has decreased the time lag to
breakdown and the minimum breakdown voltage
7
Triggering effect on water vapourisation
  • Trigger pulse with trigger pulse energies of
    1-2J and a pulse duration of 500ns means
    available power of 2-4MW
  • This energy could vaporise water and generate a
    bubble

8
Methods of examining bubble generation
1- Measurement of time lags to the main gap
breakdown, when a delay time was applied between
the trigger pulse and the main voltage 2- Optical
procedure using a photo-detector and He-Ne
laser 3- Using a conventional camera working in
the open-shutter mode 4- Using a high speed
digital camera
9
1- Time lag to the main breakdown measurement,
when a delay time was applied between the trigger
pulse and the main voltage
Time lag to breakdown vs. the delay time
,Plane-plane triggered water gap with a trigger
ring, gap voltage10kV, trigger pulse energy1J 
10
2-Schematic of reflection and refraction of laser
beam due to the presence of a gas bubble
Refractive index differences gas phase 1.006
water 1.333 means bubble acts as a divergent
spherical lens. Laser beam diverges reducing
transmitted light intensity at the detector.
11
Results from optical procedure using a
photo-detector and He-Ne laser
Intensity of a light beam transmitted through a
triggered plane-plane water gap as a function of
time after the application of a voltage pulse to
the trigger-pin
12
3- Optical procedure using a conventional camera
working in the open-shutter mode
(a)
(b) Still Pictures taken by an open
shutter camera with a trigger pulse, but without
the main gap voltage Trigger pulse energy (a)
1.44J (b) 3.26J  
13
4-An optical method using a high speed digital
camera
Successive frames at times of 200, 400, 600, and
800 ?sec showing the development of a bubble
produced in the electrode gap after the
application of a trigger pulse, energy 2.56J
14
Simulated Equipotential lines in the parallel
plane water gap including a hemisphere bubble
15
Electric field simulation in the water gap
containing a bubble using Quickfield software
16
Pre-breakdown streamer images captured by the
high-speed digital camera
Pre-breakdown streamer at the plane-plane
triggered water gap with a trigger pin, the main
gap spacing8.7mm and the main voltage16kV,
trigger pulse energy1.44J
17
Still picture from the conductive channel after
the main breakdown
Breakdown pictures taken by an open shutter
camera technique, with a main gap voltage of
16kV, gap spacing of 8.7mm and trigger pulse
energy1.44J
18
Summary
  • Bubble generation as a result of a trigger pulse
  • Electric field intensification within the bubble
  • Initiation of an electric avalanche within the
    bubble
  • Propagation of the electric streamer toward the
    high voltage electrode
  • Final breakdown in the water gap

19
Acknowledgements
I would like to thank Dr R A Fouracre and
Professor S J MacGregor for their guidance and
supervision, and also from Professor G Woolsey
for his advice and assistance during this
research. I would like to thank the Ministry of
Research, Science and Technology of Iran for
their financial support.
20
THANK YOU FOR YOUR ATTENTION AND PARTICIPATION
Msaniei_at_eee.strath.ac.uk
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