high voltage power pulse circuit
TRANSCRIPT
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7/28/2019 High Voltage Power Pulse Circuit
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IDEAS FOR DESIGN
Fast rise-time high-voltage pulseshave many uses ranging fromEMC testing to device characteri-
zation.The simple, low-cost circuit de-scribed here deals with the latter. Itsable to generate 0- to 1000-V pulseswith currents up to 50 A, and a risetime of 100 ns for 800 V/30 A. The out-
put can withstand short circuits, andcapacitive and inductive loads. Pulselength and repetition rate are deter-mined by an optically isolated TTL-in-put signal. Commercial equipment likepulse/function generators or a PC canbe connected to this input. The pulsesamplitude is set by the HV supply; alow-cost photomultiplier-type supply(0, 5 ..5 mA) can be used when repeti-tion rates are below 20 Hz.
The circuit operates as follows:when applying the HV supply, C1 ischarged up to a voltage HV via R1
and D1 (see the figure). A 0-V controlsignal keeps the PowerFET Q1 in theoff state. A 5-V signal on the controlinput operates the driver IC2, fromwhich a 12-V signal is presented onthe gate of the PowerFET Q1, bring-ing it into conductance. The output ofthe circuit becomes HV volts as the
negative terminal of C1 is nowgrounded. The pulse ends by makingthe control signal 0 V. Useful pulselength is limited by he voltage dropduring the pulse (caused by discharg-ing C1) and by the 100-s/64-A savelimit of the PowerFET. For the val-ues shown, the circuit voltage drop is10 V for a 1-s, 10-A pulse.
The short-circuit and overload pro-tection is based on R1. When the out-put current is rising, the effectivegate-source voltage of the Power-FET diminishes, enlarging the FET
resistance. With the given 0.1-value, the output current is limited to50 A. In a short-circuit situation, ca-pacitor C1 can be fully (and safely)discharged in the PowerFET. Re-verse voltages caused by inductiveloads are eliminated by D1. When the
circuit isnt operating, R14 dis-charges C1 for safety reasons.Circuit layout is very
importanta groundplane is neededto keep inductance low. C1 must be alow-inductance pulse capacitor. Eventhe FET driver IC2 needs a low-in-ductance layout and decoupling. Dur-ing the leading-edge gate currents,up to 2 A are needed to charge theFET input capacitance. Resistors R1and R2 have to be made of at least 10paralleled discretes to get a low se-
ries inductance. R4 and C3 compen-sate for the remaining inductance inR2 (the value of C3 can be changedfor this). C2, R5, R6, and R7 form asnubber network to protect the FETagainst voltage spikes. The values forthe voltage and current monitor lev-els are given for a 50- load.
Higher currents can be obtainedby duplicating the IC2-Q1-R1 stageand connecting them in parallel. R1helps to equalize the current for eachstage. A 100-A pulser has been suc-cessfully built in this manner.
High-Voltage PowerPulse Circuit
R.N. SCHOUTENFaculty of Applied Physics, DIMES, Delft University of Technology,
P.O. Box 5046, 2600A Delft, The Netherlands.
Circle 520
147
ELECTRONICDESIGN/DECEMBER1,
1997
Fast risetime pulses of 0 to 1000 V, with currents up to 50 A, can be generated by this simple, low-cost high-voltage power pulse circuit.
R447
HV Pulse output
R13330 Voltage
monitor
1 mV/V
Currentmonitor
10 mV/A
C322 nF
R34.7k
1 kV
D1RURP8100
Harris
R11330
R1556
R12330
R20.02
33
33
R6
33 2.2R7
C11F1 kV
2k
HV suppl
R18 R1410M
1200 V
C2
R5
Q1
R10.1
R82k
R92k
R10
STE16N100SGS-Thomson
+12 V
C4100 nF
10 nF
C510F
IC1
IC2
+12 V C6100 nF
R175.6k
MAX626
8
7
6
5
0/+5 V
Control In
R16200
D2
1N4148
6N135
1
2
3
48
7
6
5
1
2
3
4