Well,
I have a little better understanding after another note from a moderator over on "The Electronics Forum".
Thanks Tim, I am just starting to wrap my head around this... I just hadn't thought about it before but I guess it really has to be this way since the current draw is so high. It just wasn't intuitive to me that the screen can be higher than the plate without blocking all the signal from getting there to the plate and drawing current on the screen from the plate.
Ahh, well that only happens when the plate is around 100V. Imagine you're an electron in a tetrode or pentode. You get burned off the cathode, kind of moping around, then you find a hole in the grid, you feel more and more pull towards the screen grid, then you zip past it. (Some of your electron buddies weren't so lucky and hit a screen wire instead.) As you pass the screen, the electric field reverses and you start slowing down. But you gained so much speed approaching the screen, you're still heading smack into the plate. You get absorbed and become plate current. It's only when you really try to slow down the electrons (when Vp < 100V, so after accelerating fom the cathode and decelerating to the plate, they're going fairly slowly) that plate current drops and screen current shoots up at a dangerous rate (which suggests it's safer to have a lower load impedance than a higher load, although speakers don't allow us to be so picky). There's a little more to it than that, like secondary emission, which peaks around 50-100V in most tubes. Secondary emission is when electrons smacking the plate knock out other electrons (since, being a metal, it's holding a mess of electrons prisoner). These electrons are deflected either by adding yet another grid (the suppressor) or just by design (as in beam tetrodes). Still, it's part of the reason why tetrodes stop working in the 50-100V range specifically.
By the way, what is the 10% rule?
I don't know if anyone else said it, but I always say it.
Note some things about tubes, for instance. Their properties are all consistent within a 10% range. Say you have 300V across a resistor, well then it's drawing 1mA (apparently it was a 300kohm resistor) and dissipating 0.3W. Say it goes up to 330V (a rise of 10%); now current is at 1.1mA. Power dissipated goes up to 0.36W, which is a rise of 20%, but isn't any bother to this 1/2W resistor (oh, and it was rated for 1/2W, too). So do you care? No, not really. Hence, the Ten Percent Rule states that "differences of less than ten percent are negligible". A tube rated for 30W plate dissipation won't at all mind if you run it at 33W (except for cheapass 6L6s that start glowing red at only 25W!), or a tube that's rated for 300V running at 330.
Obviously, this does not extend to cases where you take the difference, like with a long-tailed pair or Wheatstone bridge. If one grid voltage is 100V and the other is 105V, they're close enough, right? Wrong: 105-100 = 5V, enough to turn off a 12AX7. However, it does tell you that your bias resistors (if you were to bias those grids independently, which is a bad idea for exactly the above reason) will have to hit the 100-110V range, but since you need 105.0V to balance it and you just can't guarantee that accuracy, you are going to need more refined control, such as by adding a trimmer pot.
Remember that 10% is a ratio (10% = 0.1), so it also only applies to ratios. Fortunately, lots of things can be compared as a ratio. Resistors are a unit ratio (volts per ampere), but voltage dividers are a unitless ratio (V/V or ohm/ohm) because you can compare output to input voltage, or bottom resistance to total resistance (Vo / Vi = R2 / (R1+R2) after all)....
thank you Tim,
rj
P.S. Tweedeluxe, sorry for the extensive hijack. Can we resume the direction of things toward the status on your build and how those clips are sounding.
Good, Fast, or Cheap -- Pick two...
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