> "Thévenin's ...only apply to circuits composed entirely of linear components."
Thévenin is always true.
Ok, but the equivalent "resistor" is non-linear, and therefore breaks the definition of resistor. (R=V/I) Right?
Because pure resistance is linear. But tubes are non-linear. However, their internal plate resistance is still V/I; it's just that V and I do not change at the same rate.
Look at a triode data sheet (12AX7 will do). See the plate characteristics? V on the x-axis, I on the y-axis. The grid voltage lines
are V/I, but they're curves (linear, or constant resistance, would be a straight line at some angle depending on the amount of resistance). The fundamental theory is they follow is Child's Law, or about an exponent of 3/2. That varies with the tube and operating point; non-linearity in a couple ways.
That's why PRR said Thevenin is always true, but may not be simple to calculate. It's also why tubes have characteristic curves on the data sheet, because it's easier to generate and figure the math in graphical form than in equation form.
And, because for a non-linear device V/I is not a uniform value for all V and I (that is, the ratio of the two changes because the
rate of change for each is different), you cannot use algebra to find the value of V/I. You must use ΔV/ΔI, and if the deltas get infinitely small (for a more accurate calculation) you are finding the derivative of the curve.
That's where calculus comes in, though as I said before, we don't have a handy equation for the gridlines. Each is also different (if I was a math genius, I might say the gridlines form a 3-D surface that is like a section of a cone, but I'm not that smart and I failed Calc II). Again, it's easier to perform the calculus operation of finding the derivative of the gridlines, or rate of change of the slope, through graphical means.
I understand we are dealing with a non linear system. Why is it non linear?
Well, yeah, there's the physics of it, but easier than that, you can look at the grid curves on a datasheet and see that they're curves instead of straight lines.
More than that. Pretend the gridlines are all straight. Is the tube now linear?
If the gridlines each share a common origin, but have different angles (so that they "fan out" at the extremities) then each line is a different resistance. Prove that to yourself by plotting 100Ω, 1kΩ, 10kΩ, 100kΩ on graph paper with V for x-axis and I for y-axis.
Since we know that we plot a loadline on these "curves" to show how the tube and the load divide voltage among themselves with an input signal, then if each gridline is a different resistance the tube is still non-linear. It will show a different gain on the positive input signal swing than on the negative input signal swing, because the internal resistance has changed.
So for an ideal linear tube, the gridlines must be parallel straight lines, which implies a uniform internal resistance, which is equal at every grid voltage.
Making people do the math seems to obscure the concept. Once they have the concept and they want to use it design something, they'll need to learn the math (or just be really good at breadboarding), but loading the math up front seems to be a bad idea, from what I've seen so far.
Math is a compact way to describe a complex concept that make take pages or chapters of a book. Ideally, it shows complex inter-relationships in an easy to understand fashion.
I once had a great math teacher (my Calc I teacher, as opposed to my Calc II teacher who was the worst I've ever seen anywhere). The guy was a grad student, teaching a class to help fill his degree requirements. Because he really understood the stuff he was teaching, he could break down scary looking equations into simple ideas, and help us see the overall concept it was communicating.
Don't make people do math equations, help them see graphically what the math represents. Unless you have to do proofs for a class requirement, there's probably little need in showing them how to derive each equation. The hard work is in figuring out how to make the concept simple.