@Analog Kid, for a common emitter configuration with
signal not going through the emitter resistor,
(1) a first order approximation is:
Gain ≈ V
(collector resistor) / 26 mV
This V
(collector resistor) is the average voltage we get from biasing. And that is controlled by R
E.
Be sure you paid attention. The first sentence deals with AC signal only and completely removes R
E from the image. However the equation uses V
(collector resistor), which is calculated from the opposite side, completely ignoring small-signal concerns and depending on R
E.
In other words, we first get the big picture of how things are biased. Then we apply this knowledge to the small-signal analysis.
The AGC affects biasing of the entire amplifier in a way that makes V
(collector resistor) go lower or higher. Biasing depends greatly on the resistance seen by the emitter. Be it physical resistor R
E or virtual resistance created by AGC. The circuit above can’t tell if we attached an additional resistor or are we just doing funny things with voltages.
Let’s look at a simpler version:

In this circuit DC voltage across collector resistor (R1) is about 1.27 V. From our earlier equation the gain is: 1.27 / 0.026 ≈ 48.9. Checking with simulation, it comes out as 46.6:

Now, let’s try increasing R2:
+1 kΩ (=3.2 kΩ) makes R1 voltage to be 0.902 V, and amplification of 34.7
(33.1 in sim).
+2 kΩ (=4.2 kΩ) makes R1 voltage go 0.703 V, and reduces amplification
to 27 (25.8 in sim).
+10 kΩ causes amplification to be barely 11.4, and +20 kΩ only 6.
The attachment shows waveforms for consecutive increases of emitter resistance, from bold line to dashed. Dotted is the original 2.2 kΩ.
A corresponding presentation in Paul Falstad’s simulator. Note that you may need to wait or even speed up the simulation for values to settle. See what happens, if you change R2 (slider on the right).
The rest is in my earlier post. AGC circuitry “manipulates” the amplifier into “thinking” there is a higher resistance attached to the emitter. It does that by setting voltage on one end of R
E, but the amplifier has no way of telling the difference. All it sees is that the current decreases.
⁂
So much for providing an image.
I do agree with a lot people here, that trying to understand mathematical models behind all this is relevant. The way I described it may offer nice picture answering a particular question. But you can make almost no predictions from that, if hard numbers are needed. For instance see I just given voltage on the collector resitor, but never explained why it’s this value and not some other. I said 26 mV, but why 26? Unlike others I never uttered symbols g
m and r
e. The reason I didn’t is not because they’re irrelevant, but because I wrapped them in other symbols.
(2) You’ll not see why transistor’s β plays no role, assuming it’s big enough.
On the other hand I don’t believe in bottom-top approach where bottom may be too hard to grasp all at once.
Lying to children is good.
(1) The 0.47 µF capacitor is almost a short at 1 MHz, and
is negligible for 10 kHz.
(2) The gain equation in this post is directly derived from -g
m · R
C.