Hawes Amplifier Archive by James T. Hawes, AA9DT
Improve Your Depletion FET Amp Design

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Bring Out the Best in Your FET Amplifier!

Cut & Try. Congratulations! You've designed and built a depletion-FET (or tube) amplifier, and it works. Now you need it to work even better. Maybe it doesn't have enough gain, or maybe it clips due to excessive gain. Maybe the bias works, but the drain (plate) voltage is too high or low. Maybe you want to change the frequency characteristics, reducing or increasing low or high frequencies. This page helps you to cut and try modifications until you get everything just right.

Prerequisites

  • Depletion Mode. The device must be a depletion-mode, silicon MOSFET or JFET. (No BJT transistors. No enhancement-mode MOSFETs. No GaAsFet, SiC or Ge devices.) For our examples, we'll use a Supertex LND150 MOSFET.

  • Source Bias. This technique works on source-biased ("self-biased") preamplifiers.

Diagram: Supertex LND150 in TO-92 package, showing pin layout
Supertex LND150

Definitions of FET Terms

Electrode Capacitor Resistor Voltage
Gate (Grid) Cg= Gate capacitor Rg= Gate resistor Vg= Gate voltage
Drain (Plate) Cd= Drain capacitor Rd= Drain resistor Vd= Drain voltage
Source (Cathode) Cs= Source capacitor Rs= Source resistor Vs= Source voltage
Power Cf= Filter (anti-hum) capacitor Rbl= Bleeder resistor B+= Positive power voltage (tubes)
Gnd= Ground
Vdd= Drain power voltage
Vss= Source power voltage


Gain

Resistors Set Gain

Drain & Source Resistors. If you want voltage gain (Vgain), keep RS as small as practical in relation to RD. RS must be large enough to “shove” VD up to at least half of VDD.

  • If RS is 10 percent or less of the RD value, try for this: VD = (VDD / 2).

  • If RS exceeds 1/10 of RD, try for this: VD= [(1/2VDD) + (1/2 VS)].

  • Need to reduce gain or improve fidelity? Increase your RS value.

If (RS = RD), you have a max gain of only 1. (In the real world, probably less.) If (RS > RD), your circuit is degenerative. That is, lossy. Only with (RD > RS) can you have gain. But only with VD = (1/2 or so * VDD) can you have ideal linearity.

Schematic: Increasing source resistor value decreases gain. Mouse over for advantage.

Reduce gain & boost fidelity: Increase the source resistor. (Roll over.)

Increase the Gain

Bypass the source resistor. By bypassing source resistor RS, you can use the perfect source resistor and still boost the gain. What do we mean by “bypassing”? We mean soldering a capacitor across RS. The capacitor will give a varying gain that increases as the frequency increases. On the low end, eventually the capacitor attenuates low frequencies. Larger capacitors allow lower frequencies to pass. The source capacitor formula is...

C = 1,000,000 / [2 Π * F * (RS / 10)]
Or this easier version: 160,000 / [(F * (RS / 10)]
where...
C is in microfarads.
F is in Hz.
Π is the constant pi ≈ 3.14.
RS is in Ω.

Example: For (F = 20 Hz) & (RS = 560 ohms): C = 142 μF.
Round up to a convenient standard value: 150 μF. 220 μF would also be fine.

Lower or higher cutoff. To extend the response to even lower frequencies, use a substantially larger capacitor size. To cut the low frequencies, use a substantially smaller capacitor size. (For example: If 150 μF causes rolloff at 20 Hz, 1,500 μF will cause rolloff at 2 Hz. For a 200-Hz rolloff, use 15 μF.)

Schematic: How to bypass the source resistor with a capacitor. Mouse over to connect capacitor.

Boost gain: Bypass the source resistor. (Roll over.)


Fidelity

Getting too Much Distortion?

If you hear too much distortion and want a cleaner signal, consider reducing the gain. You can decrease the gain in various ways. The easiest is just to remove the decoupling capacitor CS from source resistor RS. Afterward, you'll notice much less distortion, because RS is degenerative. This resistor feeds back a small part of the input signal, but out of phase. The out-of-phase signal counteracts distortion and makes the output signal more linear.

If you lose too much gain when you remove the source capacitor, split the source resistor. Then bypass just the bottom part of resistor. See the illustration at right. The unbypassed resistor will still cause degeneration. Yet degeneration won't be as great as with a completely unbypassed source resistor.

Potentiometer method. Some builders substitute a pot for the source resistor. The wiper (center terminal) of the pot connects to the capacitor. Then these builders can dial in some intermediate level of gain. Unfortunately, this potentiometer method adds noise to the signal.

Schematic: How to partially bypass the source resistor. Mouse over to connect capacitor.

Roll over to see partial bypass of source resistor.


Coupling Capacitors for FETs

Please see our page on Coupling Capacitors.



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WARNING. This is your project. Your achievement is entirely yours. I assume no responsibility for your success in using methods on these pages. If you fail, the same is true. I neither make nor imply any warranty. I don't guarantee the accuracy or effectiveness of these methods. Parts, skill and assembly methods vary. So will your results. Proceed at your own risk.

WARNING. Electronic projects can pose hazards. Soldering irons can burn you. Chassis paint and solder are poisons. Even with battery projects, wiring mistakes can start fires. If the schematic and description on this page baffle you, this project is too advanced. Try something else. Again, damages, injuries and errors are your responsibility. — The Webmaster



Copyright © 2011 by James T. Hawes. All rights reserved.

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