High voltage trigger-pulse generator for marxes and plasma foci
A. Robledo‐Martinez, R. Vega, Luis E. Cuéllar, A. Ruiz‐Meza, E.G. Guzman, F. Castillo, Julio Herrera
Abstract
A. Robledo‐Martinez, R. Vega, Luis E. Cuéllar, A. Ruiz‐Meza, E.G. Guzman, F. Castillo, Julio Herrera
Abstract
We report the design and implementation of a reversible, square-pulse generator for triggering spark gaps. It employs coaxial cables for charge-storage and pulse formation, and a thyratron as the switch. The generator has a nominal output voltage 5–30 kV, and a pulse length governed by the cable’s physical length. Two variants are presented: 1) single-stage one consisting of one charged cable that is discharged with a thyratron, 2) two-stage having an inverting circuit that uses a second coaxial cable to reverse the polarity of the pulse produced by the first one. Since the cables employed were wound solenoid-like special insulation was devised to avoid breakdown between adjacent coils in the winding when the pulses propagate along the shields of the cables. The rise-time obtained is mostly dictated by the switching time of the thyratron; with the one we used in the tests, rise-times in the range 30–40 ns were obtained. We present the results obtained in the application of the generator to triggering a Marx generator and a plasma focus.
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We report the design and implementation of a reversible, square-pulse generator for triggering spark gaps. It employs coaxial cables for charge-storage and pulse formation, and a thyratron as the switch. The generator has a nominal output voltage 5–30 kV, and a pulse length governed by the cable’s physical length. Two variants are presented: 1) single-stage one consisting of one charged cable that is discharged with a thyratron, 2) two-stage having an inverting circuit that uses a second coaxial cable to reverse the polarity of the pulse produced by the first one. Since the cables employed were wound solenoid-like special insulation was devised to avoid breakdown between adjacent coils in the winding when the pulses propagate along the shields of the cables. The rise-time obtained is mostly dictated by the switching time of the thyratron; with the one we used in the tests, rise-times in the range 30–40 ns were obtained. We present the results obtained in the application of the generator to triggering a Marx generator and a plasma focus.
Key concepts: Plasma, Generator (circuit theory), Voltage, Pulse generator, Pulse (music), Physics, Electrical engineering, Optoelectronics