Do you understand car or bicycle gears?
Well yes.
But I never heard the term "reflected work" when talking transmissions or pedaling my bikes. It's just work.
But you know if you pick the wrong gear in the car you lug the engine & stall. And if you pick the wrong gear on the bike going up that hill that you're not going anywhere.
I think the term "induced load" is more descriptive than "reflected load."
... there is current we control that passes through a coil of wire, and the magnetic field created by that current induces a current in all other nearby coils. ...
...
- Since Power In = Power Out, the Impedance "felt" at the Primary is the square of the Volts-change imposed by the ratio of turns between Primary & Secondary.
- ... the current induced in the Secondary has the ability to generate "back-pressure" and define the Impedance of the Primary ...
There are 2 core fallacies that people seem to apply with tube amps and output transformers, and it wrecks their ability to see how simple the power section really is:
1. The output tubes "make power."
2. The output tubes "want a certain load."
Output Tubes Pull CurrentThe output tubes is receive a grid-voltage signal and they respond by attempting to draw more/less plate current.
That's all they do.The OT Primary Impedance Creates a Voltage-DropWhen a tube pulls plate current, the current passes through the OT primary. Its primary impedance creates a voltage-drop in accordance with Ohm's Law: Volts = Current x Impedance. The voltage-drop
momentarily leaves less voltage at the tube plate.
Here, we're only thinking about the half-cycle that goes from "idle current" to "peak plate current" when thinking about the tube's plate current creating a voltage-drop across the OT primary impedance. Even so, we can understand most of what we want to know about the tube's operation from this half-cycle.
- We can acknowledge the tube's plate voltage shoots above its idle value as plate current falls below idle current and to zero-current. However, Zero-Current x Any-Voltage = Zero Power, so we care about this part of the cycle mainly with regard to transformer winding insulation.
Output Tubes Don't "Make Power"Power = Volts x Current, and our output tubes only have control over the plate current they
attempt to pull through the OT primary impedance. The resulting voltage-drop above is multiplied by the late current the tube pulled to create the voltage-drop. And
that is our power output; it's partly a byproduct of the OT primary impedance causing a voltage-drop.
- If we make the primary impedance smaller, there is a smaller voltage-drop for a given tube plate current. Power Output goes down. Power Output is being constrained by tube plate current (the tube's curves show a maximum plate current for a given condition & applied-signal).
- If we If we make the primary impedance larger, there is a larger voltage-drop for a given tube plate current. Power Output goes up,
to a limit.
- Our output tubes cannot pass plate current with 0v on their plates; typically, they need 50-100v remaining on the plate to pass current. We have a fixed supply voltage, so the most-voltage available to drop across the OT primary impedance is "Supply Volts - 100v" (or 50v or wherever the tube's "plate current knee" lands for that screen voltage).
- Going to an OT primary impedance "higher than the limit" noted above attempts to pull plate voltage down to a level that stops plate current. Power Output falls because the "Current" part of our equation is being constrained.
This image shows:
- "Optimum" loading (Blue)
- "Too-small primary impedance" loading (Red): power output is constrained by lessened voltage-swing
- "Too-large primary impedance" loading (Brown): power output is constrained by lessened current-swing