Fast rise-time high-voltage pulses have many uses ranging from EMC testing to device characterization. The simple, low-cost circuit described here deals with the latter. It’s able to generate 0- to 1000-V pulses with currents up to 50 A, and a rise time of 100 ns for 800 V/30 A. The output can withstand short circuits, and capacitive and inductive loads. Pulse length and repetition rate are determined by an optically isolated TTL-input signal. Commercial equipment like pulse/function generators or a PC can be connected to this input. The pulse’s amplitude is set by the HV supply; a low-cost photomultiplier-type supply (0, 5 ..5 mA) can be used when repetition rates are below 20 Hz.
The circuit operates as follows: when applying the HV supply, C1 is charged up to a voltage HV via R1 and D1 (see the figure). A 0-V control signal keeps the PowerFET Q1 in the off state. A 5-V signal on the control input operates the driver IC2, from which a 12-V signal is presented on the gate of the PowerFET Q1, bringing it into conductance. The output of the circuit becomes −HV volts as the negative terminal of C1 is now grounded. The pulse ends by making the control signal 0 V. Useful pulse length is limited by he voltage drop during the pulse (caused by discharging C1) and by the 100-µs/64-A save limit of the PowerFET. For the values shown, the circuit voltage drop is 10 V for a 1-µs, 10-A pulse.
The short-circuit and overload protection is based on R1. When the output current is rising, the effective gate-source voltage of the Power-FET diminishes, enlarging the FET resistance. With the given 0.1-Ω value, the output current is limited to 50 A. In a short-circuit situation, capacitor C1 can be fully (and safely) discharged in the PowerFET. Reverse voltages caused by inductive loads are eliminated by D1. When the circuit isn’t operating, R14 discharges C1 for safety reasons.
Circuit layout is very important—a groundplane is needed to keep inductance low. C1 must be a low-inductance pulse capacitor. Even the FET driver IC2 needs a low-inductance layout and decoupling. During the leading-edge gate currents, up to 2 A are needed to charge the FET input capacitance. Resistors R1 and R2 have to be made of at least 10 paralleled discretes to get a low series inductance. R4 and C3 compensate for the remaining inductance in R2 (the value of C3 can be changed for this). C2, R5, R6, and R7 form a snubber network to protect the FET against voltage spikes. The values for the voltage and current monitor levels are given for a 50-Ω load.
Higher currents can be obtained by duplicating the IC2-Q1-R1 stage and connecting them in parallel. R1 helps to equalize the current for each stage. A 100-A pulser has been successfully built in this manner.
How about a list of component values? The gif is not legible in any viewer.
Anonymous -February 10, 2008
This simple design would be superb for powering Copper vapour lasers, if it could be made to supply pulses of about 40ns rise time, width 250ns, repetion rate 15 to 20 Khz, Voltage circa 15 KV @ 1 A average current. A tall order I know, but if its possible to construct a power supply to these specs with such simple pulse forming techniques, it might be a breakthrough in terms of convenience for Copper vapour laser construction.
Vincent Borg -December 11, 2006 (Article Rating: )
This article would be extremely useful to me if the schematic was more readable or a parts list had been included. Is there any way to obtain a higher resolution schematic and/or a complete parts list? This circuit is just what I've been looking for - but I'm having to guess on a few of the component values! I wouold appreciate any help you can give me on this.
Charles Shepherd Electronic Support Facility University of North Carolina at Greensboro
Charles Shepherd -October 24, 2006 (Article Rating: )
try to improve.
Anonymous -October 11, 2006 (Article Rating: )
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