ah, i just love your posts. They are different from others. They give me an urge to study more.
You ignored the context of my comment about Ib being an annoyance. Here's what I said:Annoyance? Couldn't the same be said for Vbe? An ideal p-n junction in the forward direction has zero voltage drop for any finite current value. Second, the current controlling Ic is emitter current Ie, not base current Ib.
Thirdly, base current may not contribute directly to Ic, but it has a useful purpose. Every bjt can be fabricated for "supergain" behavior, beta value can be 4,000 to 5,000 typically. The base current exists due to hole density in the base. When b-e junction is forward biased, holes drift from base to emitter, recombining w/ emitter electrons.
The value of this hole drift is determined by the density of acceptor atoms which is controlled during the fabrication process. A sparse acceptor density & very thin base region results in great current gain values, beta. But designing the device for superbeta performance involves tradeoffs.
With thin base dimensions, & sparse acceptor density in the base, Vce blocking capability is low, & collector to base leakage current is high. Leakage from collector to base is very undesirable, it hurts performance while providing no benefit. Also, punch through when Vce breakdown occurs is very undesirable.
So how we avoid these 2 bad behavior issues, is to increase doping density of acceptor atoms in the base region (npn device), which reduces c-b leakage current, & widen base region, which increases Vce blocking ability. The price paid is lower beta & higher base current, but it is worth it. Again, Ib does not directly contribute to Ic, but it mitigates these 2 problems I discussed.
I would rather have a bjt that required a little more base current but exhibits less c-b leakage, as well as not exhibit Vce punch-through. I'm sure you don't want those either.
Likewise, Vbe is an annoyance. In logic, output swing for an emitter follower cannot go to the rail because of Vbe. If Vbe were 0.01 V, life would be better. A power amplifier exhibits crossover distortion because of Vbe value of 0.7V. If it were 0, crossover would have lower distortion.
Germanium bjt devices have lower Vbe, a desirable feature. But their collector-base leakage current is much greater than silicon, esp at high temp. With Si, we accept the higher Vbe in return for better c-b leakage current values. It's a tradeoff indeed.
Finally, if a bjt amp stage is configured as an emitter follower, a common use, Ib combines with Ic & Ie is the load current. In an EF, Ib is not going to waste, it drives the load. Many standard npn linear regulators use an EF stage for the output. The low dropout regulators use either a pnp bjt or P MOSFET stage. The configuration is common emitter or common source. With CE, Ib does not drive the load.
Anyway, I had to clear up this urban myth that Ib is just an annoyance. I studied semiconductor physics including fabrication, & believe me, if we have had the ability to produce bjt parts with beta of 5,000 since the 60's, but we generally opt not to, you know there is a good reason. If higher base current was merely an annoyance, it would have been reduced in every device to the extent feasible.
OEM producers of bjt intentionally lower beta, & increase base current, because there is something to be gained by doing so. Higher acceptor atom density reduces c-b leakage, & longer base region distance increases Vce blocking value. These are good things - I'm sure you would agree. BR.
Claude
In op amps, Ib is an annoyance.Differential amplifiers, the heart of op amps, are basically (IMHO) voltage-controlled devices. The base current is an annoyance that has to be dealt with, or at least accounted for.
I just explained that in op amps, superbeta devices are used in front end to minimize Ib. The input to an op amp need not withstand high Vce values. The leakage current c-b is minimized by a servo loop that forces Vbc to near zero volts. Just as Ib can be regarded as an annoyance, so can Vbe & Vbc.You ignored the context of my comment about Ib being an annoyance. Here's what I said: In op amps, Ib is an annoyance.
Why can't we just say that CB leakage is also an annoyance?
And I don't agree that Ib driving the load in an emitter follower is a plus. In most usages of emitter followers, the goal is to reduce loading on the source. Ib loads the source.
Maybe they should start adding gate current to FETs. Think of all the advantages.![]()
Apparently you don't recognize sarcasm. I even added rolled eyes after my question about adding gate current to FETs, to signify such.Why don't we add gate current to a FET? Because nothing is gained, at least as far as conduction current goes. But making the g-s capacitance larger increases gm, the transconductance (id/vgs). So we are in fact adding current to the gate. Another classic tradeoff. Increasing gm results in more g-s capacitance, & more gate current. Some applications favor this, some do not.
Well stated Ron, I do agree with that statement in its entirety. I also wish to add that a board level circuit design engineer is not going to say "thank God for Vbe!" Again, Vbe cannot be removed, so let's deal with it in a manner similar to other parameters, making tradeoffs as needed, depending upon which parameters are more important for the task at hand.Thanks for the core dumps.
Apparently you don't recognize sarcasm. I even added rolled eyes after my question about adding gate current to FETs, to signify such.
To a semiconductor physicist or design engineer, Ib is apparently a useful tool.
I don't think you will ever find a board-level circuit design engineer saying "Thank God for base current!".