high voltage power pulse circuit

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  • 7/28/2019 High Voltage Power Pulse Circuit

    1/1

    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