JFET bias calculations

Started by demonstar, April 27, 2008, 07:52:43 AM

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demonstar

I think after trawling through and through past posts here and articles elsewhere I am well on my way to understanding this but I've come a bit stuck piecing it all together. I was hoping maybe you guys could give me a hand? Here goes...

I have a JFET that is setup in a common source configuration as follows... it has a source resistor (RS), a drain resistor (RD) and a gate resistor (RG). The drain resistor is 1M which I gather to be standard (believe this is chosen for a suitably high impedance whilst low enough to prevent oscillations).

In this set up I understand that the gate resistor is attaching the gate to ground making VG zero. This then means as VCC causes ID to flow through RS a voltage is developed across RS equal to VS=IDRS. This then means as the gate is being held at zero volts, VS is now above VG. So VG is negative. This means ID is being restricted by the negative VGS. This means ID is now set. Now we would have to apportion the drain resistors size depending on desired output impedance, the stages gain and headroom. For equal headroom RD+RS=4.5/ID because that would set VDS to 4.5V, right?

How does that sound? What I'd like to know is how do I actually calculate the bias point? I think I am armed with the equations and the verbal explanation just can't piece the two together.

Does a JFET have a VGS(TH) like a MOSFET or like the the bipolar diode drop that needs accounting for?
The equations I believe I'd need are...
RD+RS=4.5/ID
RD=(4.5/ID)-RS
VGS=VG-VS but since VG=0 then VGS=-VS
Av=RD/RS
VS=ID*RS
VD=ID*RD
Av=vout/vin so Av=vd/vg

Thanks!
"If A is success in life, then A equals x plus y plus z. Work is x; y is play; and z is keeping your mouth shut"  Words of Albert Einstein

R.G.

The reason you haven't seen a simple explanation of this is that there isn't a good, simple one. Well, there may be one, but I've never found it. 

JFETs do not have a Vth in the sense that MOSFETs do. Well, OK, they do, but it's negative. JFETs can't simply be biased by the emitter/source-follows-the-base/gate method because the turn on/off range on the gate is so large. The exceptions are the few JFETs like the J201s which have a Vgsoff of only less than a fraction of a volt. That could be coped with, but then the range of full-off to full-on varies by 3:1 to as much as 5:1.

There are graphical methods for achieving a reasonably small solution to biasing JFETs. Vishay/Siliconix had one it published, and no doubt someone has the link. I read it, didn't find it much use so I didn't bother to remember it in detail.
R.G.

In response to the questions in the forum - PCB Layout for Musical Effects is available from The Book Patch. Search "PCB Layout" and it ought to appear.

demonstar

Thanks R.G.

QuoteThe reason you haven't seen a simple explanation of this is that there isn't a good, simple one
Guess that makes you the bringer of bad news today.  :(

QuoteThere are graphical methods for achieving a reasonably small solution to biasing JFETs. Vishay/Siliconix had one it published, and no doubt someone has the link. I read it, didn't find it much use so I didn't bother to remember it in detail.
I think I may have seen that. I have certainly read articles on the graphical method. I don't really like the graphical stuff because I think quite often in the very small currents and voltages we operate at it can be very hard to read off the graphs reliably.

You mention that there isn't a simple explanation well how not so simple is the not so simple version? :D
Is it worth learning or should I consider JFETs an art not a science? What I'm saying is the not so simple method in reach of an AS-level student?

Thankyou!
"If A is success in life, then A equals x plus y plus z. Work is x; y is play; and z is keeping your mouth shut"  Words of Albert Einstein

brett

QuoteThe drain resistor is 1M

That should be Gate resistor.  Yes?

The application note that RG mentions is educational, but doesn't spend much time discussing the "self-biasing" systems that we use here.  It spend lots of time on things like "Vref" systems where a fixed bias is applied to the gate.

Good luck with your quest.
Brett Robinson
Let a hundred flowers bloom, let a hundred schools of thought contend. (Mao Zedong)

demonstar

Yeah Brett thanks. Just made a typo. I'm going to try and seek that text out and read it. I've got a transistor principles book by Amos coping from ebay so I'm hoping that might have some info. on this subject in.
"If A is success in life, then A equals x plus y plus z. Work is x; y is play; and z is keeping your mouth shut"  Words of Albert Einstein

brett

3 handy JFET articles, especially wrt biasing:
Siliconix AN102 - biasing JFETs
FET principles and circuits, Parts 1 to 4, by Ray Marston.  Nuts and Volts Magazine, 2000.
JFETs: the new frontier, Part 1 by Erno Borbely.  Audio Electronics 5/1999.

All of these are available on-line.
cheers
Brett Robinson
Let a hundred flowers bloom, let a hundred schools of thought contend. (Mao Zedong)

demonstar

I just wanted to say thankyou folks for pointing me in the right direction and helpping me out. I couldn't find the nuts and volts article but apart from that I found the other two. The Erno Borbely article was particularly good. It has really helped. There were a couple of things such as THD that I have never heard of and don't understand but apart from that it was great.

I'm hoping a 'Principles or Transistor Circuits', by S.W. Amos that I am waiting for in the post that should come soon will be good!   :icon_smile:
"If A is success in life, then A equals x plus y plus z. Work is x; y is play; and z is keeping your mouth shut"  Words of Albert Einstein

brett

THD = total harmonic distortion.  Hi-fi people want to reduce it to zero, but we guitarists want it in certain amounts and flavours. (ie where would AC/DC be without lots of it?)

As for the thanks.... what goes around comes around, so it's a pleasure.
Brett Robinson
Let a hundred flowers bloom, let a hundred schools of thought contend. (Mao Zedong)