Secondary winding potential distribution of Tesla transformer

zhang xi-bo; su jian-cang; peng jian-chang; song xiao-xin; wang li-min; pan ya-feng

Volume 20 Issue 09

Sep. 2008

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Article Navigation > High Power Laser and Particle Beams > 2008 > 20(09): 0-

niu hong-chang, qian bao-liang. Particle simulation of compact L-band coaxial relativistic backward wave oscillator[J]. High Power Laser and Particle Beams, 2006, 18.

Citation:

zhang xi-bo, su jian-cang, peng jian-chang, et al. Secondary winding potential distribution of Tesla transformer[J]. High Power Laser and Particle Beams, 2008, 20.

niu hong-chang, qian bao-liang. Particle simulation of compact L-band coaxial relativistic backward wave oscillator[J]. High Power Laser and Particle Beams, 2006, 18.

Citation:

zhang xi-bo, su jian-cang, peng jian-chang, et al. Secondary winding potential distribution of Tesla transformer[J]. High Power Laser and Particle Beams, 2008, 20.

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Secondary winding potential distribution of Tesla transformer

1.
Northwest Institute of Nuclear Technology,P.O.Box 69-13,Xi’an 710024,China

Publish Date: 2008-09-15

Abstract

Abstract

A non-uniform parameter double-transmission-line model is created to explore the voltage distribution in Tesla-transformer taper windings. With the method of differential approximation, the numerical results are shown that during the charging process of PFL, the maximal electric-field intensity moves gradually from the small-radius end to the large-radius end, whereas during the discharging process and the abnormal discharging process of PFL, the maximal electric-field intensity is on the large-radius end. What’s more, the maximal electrical field intensity of the three processes, which happens in the abnormal discharging process of PFL, is approximately 1.5 times the average electric-field intensity.
- pulsed power technology,
- tesla transformer,
- secondary windings,
- potential distribution,
- double-transmission-line model

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