3. The cornell note format calls for the left hand column to be 2-1/2 wide, This column width could be violated, but then we have to call it "modified Cornell Note Format"
If the format is being used to aid in understanding, then slavish adherence to the format
when it impedes understanding seems counterproductive.
A second problem is that tube manual examples are carefully crafted to match optimum conditions previously worked out. When you re-apply the process to real-life situations, you can correctly get an answer which turns out to not be the "best" or "right" answer, even though the stesp were all executed correctly. So you might have to make multiple iterations, and these slop-up the note format further.
Which brings up the 2A3 issue:
I lost a reply when I added this.
Known sources of error in the posting.
1. RC-30 would make a n bias volt adjustment, for the 2A3, if filament voltage is ac. If you argue, that the 12AU7, was an indirect heated, and did not need the adjustment. I can see your argument.
Yep, that's the big one. For others following, the 2A3 is a
filamentary, or "directly-heated," power triode which means its filament is also its cathode. They are not separate structures. The 12A_7 series is instead a heater/cathode type tube, where these are separate structures.
Technically, if you see "filament" it implies a tube that is directly-heated like the 2A3. These are very uncommon today, so heater and filament are often interchangeable. The problem is if a directly-heated tube is fed a.c. to light the filament, it may interfere with bias since the filament is also the cathode. So these circuits would use a filament winding with a center-tap, and the total bias had to be increased by half of the filament voltage as it was inseparable from the cathode voltage.
Now the impact of this discrepancy is bigger than you'd think. The 2A3 has a filament voltage of 2.5v, which means a half-voltage increase of bias is a change of 1.25v. You can see from data sheets (and the example here) that bias is in the range of -40 to -45v, or about a 3% change in bias.
The example adjusted the 12AU7 bias for a.c. by adding 1.7v of bias (unrelated to the tube's a.c. heater voltage of 6.3v?) to go from -13.3v to -15v. That's a 12.7% change of bias, as we're talking about a tube with a much smaller bias voltage (because its mu is well above that of the 2A3).
I'd also argue the calculated mu should be different. We have to cheat from the answers to know, but from the
Firefly schematic we see that 12AU7 plate current should be 0.5 * 8.8v / 440Ω = 10mA. The Firefly also shows B+ as 265v, with 8.8v across the cathode resistor, or ~250v as the supply voltage. Your example cited ET-T880A, and we should focus on the graph on page 3 of the
G.E. 12AU7A data sheet. It shows that mu changes with both supply voltage and
especially plate current, so using the Eb=250v curve and 10mA of plate current, mu is given as ~16.8.
The result of those 2 changes is that bias should be ~-10.1v, which raises the loadline closer to the plate dissipation curve. That the line was so far from the plate dissiaption curve should have been a clue that the calculation couldn't be correct for optimum power output. However, even my calculated numbers don't jive with the reality of the Firefly, which then suggests that the formula just gives a starting point, which the user must refine. It's too bad it doesn't sync well with the 12AU7.