JFET-based dc/dc converter operates from 300-mV supply
By Jim Williams, Linear Technology Corp, Milpitas, CA; Edited by Brad Thompson and Fran Granville -- 5/25/2006
You use a JFET's self-biasing characteristics to build a dc/dc converter that operates from power sources such as solar cells, thermopiles, and single-stage fuel cells, all of which deliver less than 600 mV and sometimes as little as 300 mV. Figure 1 shows the drain-to-source characteristics of an N-channel JFET under zero-bias conditions, which you can produce by connecting its gate and source together. Applying 100 mV causes a current of 10 mA to flow through the device, increasing to 30 mA at 350 mV. Exploiting the JFET's ability to conduct significant current at zero bias makes it possible to design a self-starting, low-input-voltage converter.
The circuit can supply 5V at currents as large as 2 mA—enough to serve many micropowered applications or to provide auxiliary bias for a higher power switched-mode voltage regulator. At 300-mV input, the circuit starts up at load currents of 300 µA. A load current of 2 mA requires an input of 475 mV.
In Figure 2, Q1, a parallel-connected pair of Philips Semiconductor's (www.semiconductors.philips.com) BF862 JFETs, and Coiltronics' (www.coiltronics.com) Versa-Pac transformer, T1, form an oscillator in which T1's secondary winding provides feedback to Q1's gate. When you first apply power, Q1's gate rests at 0V, and drain current flows through T1's primary winding. T1's phase-inverted secondary winding responds by delivering a negative voltage to Q1's gate, which turns off Q1 and interrupts current flow through T1's primary winding. In turn, T1's secondary voltage collapses, and sustained oscillations begin. Although the BF862's published specifications do not cover the device's internal geometry, the device has a low on-resistance and maintains a low gate-turn-on threshold voltage. Using a pair of parallel-connected JFETs for Q1 ensures the low saturation voltage for operation at low power-supply voltages.
Rectifying and filtering the positive-going flyback-voltage impulses on Q1's drain produce a dc voltage across capacitor C1. To assist the circuit's start-up, a P-channel MOSFET, Q2, which requires a gate-to-source voltage of approximately 2V for conduction, initially isolates the output load from the rectifier. When Q2 conducts, the output voltage increases toward 5V. Comparator IC1, a Linear Technology (www.linear.com) LTC-1440, draws power from Q2's source and imposes output-voltage regulation by comparing its internal voltage reference with a sample of the output voltage. The output from IC1 varies Q1's on-time through Q3 to close the control loop and maintain output-voltage regulation. Figure 3 shows the ripple voltage present at the power supply's output. When the output voltage decays, comparator IC1 switches (Trace B, middle) and allows Q1 to oscillate. The resulting flyback events at Q1's drain (Trace C, bottom) restore the output voltage.
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