Another x-Chapters section to read and think about. Here's 2x.11 where we take up BJT high-frequency bandwidth limits, Ccb, fT, etc. I've also included the two preceding sections, 2x.9 and 2x.10, but we didn't have the time (or maybe also the inclination) to do much with those. I'm primarily interested in your comments on section 2x.11, it's a useful topic, and I hope we properly understand it, and are clear. My interests peak a little ways below the real true RF region, so no s-parameters, or any of that stuff.
AoE x-Chapters - 2x.11 BJT bandwidth, fT
The 2N3904 looks like Mom's meatloaf or the Cleveland Brown's aspirations as a team, in transistor form. It's not fancy or nothin' but when filet mignon isn't available or too expensive it won't do ya wrong
P 135, I've seen lots of transistors ocillate with a well-bypassed collector. That's not always a fix. A base resistor apparently is.
Wire bonds are evil.
More interesting stuff, thanks.
You might want to add another sentence to the discussion of high-level injection effects on beta--the origin of the base current is recombination, which goes as the product of the electron and hole densities. HLE is when injected carrier density >~= doping density, resulting in enhanced recombination and so lower beta.
A Hartley oscillator is a Colpitts made by tapping the tank inductor instead of the capacitor, and there's no tapped element in your circuit. The emitter-follower oscillator is a negative-resistance oscillator, which is why adding base resistance fixes it.
You might mention Carl Battjes' fT doubler, in which each side of a diff pair has two transistors with their bases wired in series and their collectors in parallel. (Battjes has a chapter in one of Jim Williams's books, entitled "Who wakes the bugler?".)
Cheers
Phil Hobbs
Yes, I am not at all convinced that a high impedance at the collector is necessary for an emitter follower to oscillate. If there is a capacitive load on the output (emitter) then I think that it can make the input impedance have a negative real part.
I found this document interesting, though I cannot claim to have understood it fully yet:
An emitter follower with well bypassed base and collector, and just a resistive pulldown on the emitter, will often oscillate.
That guy does a lot of impressive-looking math and ignores the leads and wire bonds.
Well, with some inductive feedback allowed between emitter or collector current and the base wiring, you'll get over-unity gain sometimes. It's usually voltage slew capacitor coupled that gets 'bypassed'. A resistor in the base lead is the R-L filter component you need, sometimes.
Either that, or careful wire placement.
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