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Streamer discharges in High magnetic fields F. Manders 1 , P. Christianen 2 , J. Maan 2 1: Philips Lighting B.V., Advanced Development Lighting, P.O. Box 80020, 5600 JM Eindhoven, The Netherlands 2: University of Nijmegen, high field magnet laboratory, Toernooiveld 7, 6525 ED Nijmegen, The Netherlands model Experimental results There is a Lorentz force on a charged particle F = q(E + v x B) constant drift, perpendicular to B and E The drift motion for particle with a collision time mv = -eE – ev x B – mv/ rewriting to: tan eB/m In a pure radial electric field a particle always makes the same Hall angle with the local, radial directed electric field Introduction nt to plate measurements in nitrogen with –40 kV All experiments are done in a nitrogen atmosphere with a point to plate geometry. The distance between the point and plate is 15 mm. We used a ICCD camera which has a gate time of 5 nsec. and it can only take one image per discharge. With a good timing it is possible to gate the camera in such a way that we can see the starting of the discharge and by changing the delay time follow the whole development of the discharge as can be seen in figure to the left side. Results without magnetic field The higher the pressure the slower the discharge The higher the pressure the more branching The lower the pressure the more diffuse the streamer tip is (see the figure on the left side at 200 Torr) Negative streamers branch more then positive streamers 200 Torr , -40 kV different magnetic fields 400 Torr -40 kV magnetic fields different direction The calculated paths for a streamer for different H and the measured path The calculated paths for a streamer for different H and the measured path 400 Torr positive voltage 40 kV T T Changing magnetic field direction, chances the direction of the curvature Changing direction of the electric field, has no influence Amplitude of the electric field has no influence on the curvature It is possible to simulated the streamer path by calculating the direction of the electric field in every point and adding Conclusions The path of a streamer in magnetic field can be described by a particle which always makes the same Hall angle with the local, radial directed electric field Field enhancement after streamer formation indeed leads to a new propagation direction Photoionization does not play a mayor role in the direction where the discharge is growing, otherwise the discharge would go straight ahead in a magnetic field (magnetic field does not have any influences on Photons) More details see: http://webdoc.ubn.kun.nl/mono/m/manders_g/condtoint.pdf

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Introduction. Point to plate measurements in nitrogen with –40 kV. - PowerPoint PPT Presentation

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Streamer discharges in High magnetic fields F. Manders1, P. Christianen2, J. Maan2

1: Philips Lighting B.V., Advanced Development Lighting, P.O. Box 80020, 5600 JM Eindhoven, The Netherlands2: University of Nijmegen, high field magnet laboratory, Toernooiveld 7, 6525 ED Nijmegen, The Netherlands

model

Experimental results

•There is a Lorentz force on a charged particle

F = q(E + v x B)

• constant drift, perpendicular to B and E

The drift motion for particle with a collision time mv = -eE – ev x B – mv/

rewriting to:

taneB/m

In a pure radial electric field a particle always makes the same Hall angle with the local, radial directed electric field

Introduction Point to plate measurements in nitrogen with –40 kV

All experiments are done in a nitrogen atmosphere with a point to plate geometry. The distance between the point and plate is 15 mm. We used a ICCD camera which has a gate time of 5 nsec. and it can only take one image per discharge. With a good timing it is possible to gate the camera in such a way that we can see the starting of the discharge and by changing the delay time follow the whole development of the discharge as can be seen in figure to the left side.

Results without magnetic field • The higher the pressure the slower the discharge• The higher the pressure the more branching• The lower the pressure the more diffuse the streamer tip is (see the figure on the left side at 200 Torr)• Negative streamers branch more then positive streamers

200 Torr , -40 kV different magnetic fields

400 Torr -40 kV magnetic fields different direction

The calculated paths for a streamer for different H and the measured path

The calculated paths for a streamer for different H and the measured path

400 Torr positive voltage 40 kV

T

T

• Changing magnetic field direction, chances the direction of the curvature• Changing direction of the electric field, has no influence• Amplitude of the electric field has no influence on the curvature• It is possible to simulated the streamer path by calculating the direction of the electric field in every point and adding

Conclusions •The path of a streamer in magnetic field can be described by a particle which always makes the same Hall angle with the local, radial directed electric field• Field enhancement after streamer formation indeed leads to a new propagation direction•Photoionization does not play a mayor role in the direction where the discharge is growing, otherwise the discharge would go straight ahead in a magnetic field (magnetic field does not have any influences on Photons)More details see: http://webdoc.ubn.kun.nl/mono/m/manders_g/condtoint.pdf