Design and Development of a Line-Type Pulsed Modulator Driver for S-Magnetron for Microwave–Plasma Interaction Experiments in SYMPLE

System for microwave–plasma experiments (SYMPLEs) is an experimental system setup in our laboratory for investigating the interaction of high-power microwave (HPM) with overdense plasma with plasma frequency <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$f_{\mathrm { pe}} \gt f_{\mu }$</tex-math> </inline-formula>, the wave frequency. The washer-gun plasma chosen for these experiments is pulsed (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$100~\mu $</tex-math> </inline-formula>s) and is operated in single-shot mode. The experimental campaign involves the excitation and launching of a pulsed (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$5~\mu $</tex-math> </inline-formula>s) microwave output from an S-Magnetron to the plasma at a predecided temporal regime where the plasma parameters satisfy the required critical requisites for the wave plasma interaction. Therefore it is necessary that the magnetron source is operated in single-shot mode, and the HPM output of all such shots is highly repetitive. The pulsed power driver for the magnetron should thus be capable of giving out highly reproducible (within ±5%) single-shot trapezoidal pulses of maximum 52 kV and 120 A current, with <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$5~\mu \text {s}$</tex-math> </inline-formula> flat top and about 5%–10% rise time, consistent with the requirement of the magnetron. As conventional solid-state modulators pose challenges in achieving shot-to-shot repeatability in single-shot operation, a pulse-forming network (PFN)-based modulator has been chosen despite the stringent pulse rise time requirements. A Guillemin Type-E line-type pulsed modulator has been designed, simulated, and developed indigenously in our laboratory. The design consideration includes the incorporation of a pulse transformer at the output of the pulsed modulator, with the magnetron load impedance of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$433.33~\Omega $</tex-math> </inline-formula> constituting the secondary impedance. The primary impedance of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$25~\Omega $</tex-math> </inline-formula> is treated as the load impedance for the pulsed modulator. The design approach has involved theoretical estimation of the per-section capacitance, inductance, and coupling coefficient values followed by simulation to determine the best suitable parameters for the 10-stage PFN. A setup consisting mainly of a high-voltage dc charging unit, the 10-stage PFN, a thyratron switch with an appropriate trigger module, and a pulse transformer withbifilar secondary windings has been developed and tested with dummy loads. Experimental results on dummy loads up to 35 kV output give highly reproducible (within ±5%) voltage and current pulses of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$5~\mu \text {s}$</tex-math> </inline-formula> flat top and about 300–500 ns rise time. Details of the design, simulation, development, and test results of the line-type pulsed modulator are discussed in this article.

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Journal
IEEE Transactions on Plasma Science
Published
2025-06-17
DOI
https://doi.org/10.1109/tps.2025.3575896
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1
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Gyrotron and Vacuum Electronics Research
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article
Field-Weighted Citation Impact
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article

Design and Development of a Line-Type Pulsed Modulator Driver for S-Magnetron for Microwave–Plasma Interaction Experiments in SYMPLE

Priyavandana J. Rathod, V. Anitha
1 citations
IEEE Transactions on Plasma Science
Gyrotron and Vacuum Electronics Research
1.25
article

Design and Development of a Line-Type Pulsed Modulator Driver for S-Magnetron for Microwave–Plasma Interaction Experiments in SYMPLE

Priyavandana J. Rathod, V. Anitha
article en
1 citations

Abstract

System for microwave–plasma experiments (SYMPLEs) is an experimental system setup in our laboratory for investigating the interaction of high-power microwave (HPM) with overdense plasma with plasma frequency <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$f_{\mathrm { pe}} \gt f_{\mu }$</tex-math> </inline-formula>, the wave frequency. The washer-gun plasma chosen for these experiments is pulsed (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$100~\mu $</tex-math> </inline-formula>s) and is operated in single-shot mode. The experimental campaign involves the excitation and launching of a pulsed (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$5~\mu $</tex-math> </inline-formula>s) microwave output from an S-Magnetron to the plasma at a predecided temporal regime where the plasma parameters satisfy the required critical requisites for the wave plasma interaction. Therefore it is necessary that the magnetron source is operated in single-shot mode, and the HPM output of all such shots is highly repetitive. The pulsed power driver for the magnetron should thus be capable of giving out highly reproducible (within ±5%) single-shot trapezoidal pulses of maximum 52 kV and 120 A current, with <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$5~\mu \text {s}$</tex-math> </inline-formula> flat top and about 5%–10% rise time, consistent with the requirement of the magnetron. As conventional solid-state modulators pose challenges in achieving shot-to-shot repeatability in single-shot operation, a pulse-forming network (PFN)-based modulator has been chosen despite the stringent pulse rise time requirements. A Guillemin Type-E line-type pulsed modulator has been designed, simulated, and developed indigenously in our laboratory. The design consideration includes the incorporation of a pulse transformer at the output of the pulsed modulator, with the magnetron load impedance of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$433.33~\Omega $</tex-math> </inline-formula> constituting the secondary impedance. The primary impedance of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$25~\Omega $</tex-math> </inline-formula> is treated as the load impedance for the pulsed modulator. The design approach has involved theoretical estimation of the per-section capacitance, inductance, and coupling coefficient values followed by simulation to determine the best suitable parameters for the 10-stage PFN. A setup consisting mainly of a high-voltage dc charging unit, the 10-stage PFN, a thyratron switch with an appropriate trigger module, and a pulse transformer withbifilar secondary windings has been developed and tested with dummy loads. Experimental results on dummy loads up to 35 kV output give highly reproducible (within ±5%) voltage and current pulses of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$5~\mu \text {s}$</tex-math> </inline-formula> flat top and about 300–500 ns rise time. Details of the design, simulation, development, and test results of the line-type pulsed modulator are discussed in this article.

IEEE Transactions on Plasma ScienceVol. 53(7)
Homi Bhabha National Institute (IN), Institute for Plasma Research (IN)
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Gyrotron and Vacuum Electronics Research
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