Originally posted by Enzo
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Nope, TIP 31 and TIP 32 are plain old bipolars.
regardless, single or darlington, they are pass transistors, the zener at the base of each sets a voltage, which the emitter follows. Et voila, voltage regulator.Education is what you're left with after you have forgotten what you have learned.
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Originally posted by Enzo View PostNope, TIP 31 and TIP 32 are plain old bipolars.
regardless, single or darlington, they are pass transistors, the zener at the base of each sets a voltage, which the emitter follows. Et voila, voltage regulator.If I have a 50% chance of guessing the right answer, I guess wrong 80% of the time.
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What I find interesting about the schematic Enzo posted is the dual N-channel output with a bootstrap (C6) so Q4 cab saturate.WARNING! Musical Instrument amplifiers contain lethal voltages and can retain them even when unplugged. Refer service to qualified personnel.
REMEMBER: Everybody knows that smokin' ain't allowed in school !
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Originally posted by loudthud View PostWhat I find interesting about the schematic Enzo posted is the dual N-channel output with a bootstrap (C6) so Q4 cab saturate.If I have a 50% chance of guessing the right answer, I guess wrong 80% of the time.
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Originally posted by SoulFetish View PostYeah that's weird. Does that cap have no effect on Q5?
Q5 is not used (NU) in this particular amp. It was probably included on the schematic just for the PCB layout. Another amp might use Q4 and Q5 to achieve more output and use the same PCB. C6 pushes the supply for Q1 and Q3 above the V+ rail so that the extra 5V or so is available to turn Q4 fully on. Q1 and Q3 don't mind the little nudge they get form C6 because their Collector impedance is quite high. If the Gate Voltage of Q4 could only go to the rail, the positive output could only go up to about V+ minus the threshold of Q4 (when driving a resistive load). It's really just a trick to eliminate the need for a separate power supply. Q6 doesn't have this problem because it's Source is tied to the V- rail. Some MOSFET complementary source follower designs just throw away the extra output swing (and power) they could get and let the output clip softly.WARNING! Musical Instrument amplifiers contain lethal voltages and can retain them even when unplugged. Refer service to qualified personnel.
REMEMBER: Everybody knows that smokin' ain't allowed in school !
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Originally posted by Malcolm Irving View PostAfter two cathode-bypassed gain stages, I think blocking would indeed normally be an issue at the V2A stage.
The partial cathode-bypassing of stages V1A and V1B, and the low value coupling cap (0.0047uF) to V2A, all give some bass cut (I think - without doing any calculations) which is good when blocking might be an issue later in the circuit.
With the large 470k grid stopper on V2A, combined with the 220k to make up the grid leak, you get a good balance between the charging and discharging time constants for the 0.0047uF coupling cap – again a good measure against blocking.
If we take the output impedance of the V1B stage as (say) 40k, the charging time constant when the grid is conducting is approx.
( 40k + 100k + 470k||220k ) x 0.0047 e-6 = 1.36mS
And for discharging (when the grid is not conducting):
( 40k + 100K + 220k ) x 0.0047 e-6 = 1.69mS
It’s a nice design, in my opinion.
You could reduce the grid stop value. Which would add a little gain so you could then reduce the load resistance even further, again necessitating a change of the coupling cap value. And so on...
I'd bet that a simple .02uf coupling cap, a 47k load and a 10k grid stop would give better results with a small increase in gain.Last edited by Chuck H; 10-08-2016, 03:37 AM."Take two placebos, works twice as well." Enzo
"Now get off my lawn with your silicooties and boom-chucka speakers and computers masquerading as amplifiers" Justin Thomas
"If you're not interested in opinions and the experience of others, why even start a thread?
You can't just expect consent." Helmholtz
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Originally posted by Chuck H View PostWithout doing the math... You could actually omit the voltage divider. Just use a 58k load against the tubes internal resistance. Because of the lower impedance you'd need to bump the coupling cap to .017uf to maintain the same knee frequency. But this should still reduce the time constant even further. Then...
You could reduce the grid stop value. Which would add a little gain so you could then reduce the load resistance even further, again necessitating a change of the coupling cap value. And so on...
I'd bet that a simple .02uf coupling cap, a 47k load and a 10k grid stop would give better results with no reduction in gain.
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Well... I like eloquence in design. Playing the tubes internal resistance against the load rather than employing a component resistor voltage divider omits one part AND reduces impedance (and therefor time constant) on a circuit that could use a lower time constant anyway. Eloquence. Fewer parts and more goal oriented
Sorry?"Take two placebos, works twice as well." Enzo
"Now get off my lawn with your silicooties and boom-chucka speakers and computers masquerading as amplifiers" Justin Thomas
"If you're not interested in opinions and the experience of others, why even start a thread?
You can't just expect consent." Helmholtz
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Originally posted by Chuck H View PostWell... I like eloquence in design. Playing the tubes internal resistance against the load rather than employing a component resistor voltage divider omits one part AND reduces impedance (and therefor time constant) on a circuit that could use a lower time constant anyway. Eloquence. Fewer parts and more goal oriented
Sorry?
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I've been screwing with it since i last posted. Yeah....i'm hopeless. It's like a giant jigsaw puzzled and i can't stop till theres nothing more to gain. Anyways, i have been playing around with your idea and i now think i may like it. Gotta wait till tomorrow because it's late but i think i like the articulation more than the schematic, and thats real important because it has a huge effect on my playing. Just may need to change some other things to accommodate the different sound like treble peaker and gain pot bleed values. We shall see...
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Did you remove the 100k series resistor?"Take two placebos, works twice as well." Enzo
"Now get off my lawn with your silicooties and boom-chucka speakers and computers masquerading as amplifiers" Justin Thomas
"If you're not interested in opinions and the experience of others, why even start a thread?
You can't just expect consent." Helmholtz
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Originally posted by daz View PostI've been screwing with it since i last posted. Yeah....i'm hopeless. It's like a giant jigsaw puzzled and i can't stop till theres nothing more to gain. Anyways, i have been playing around with your idea and i now think i may like it. Gotta wait till tomorrow because it's late but i think i like the articulation more than the schematic, and thats real important because it has a huge effect on my playing. Just may need to change some other things to accommodate the different sound like treble peaker and gain pot bleed values. We shall see..."Take two placebos, works twice as well." Enzo
"Now get off my lawn with your silicooties and boom-chucka speakers and computers masquerading as amplifiers" Justin Thomas
"If you're not interested in opinions and the experience of others, why even start a thread?
You can't just expect consent." Helmholtz
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Originally posted by Chuck H View PostThe lower impedance accounts for the greater articulation. The higher the impedance, the greater the effect of impedance rising with frequency. With the lower impedance circuit there will be more balance across the audible range. That is, less loss at higher frequencies. I expected this affect and wondered if you might like it or not. Sometimes, Especially WRT guitar amps, it's actually good to have a circuit induced HF roll off. It avoids the un-aesthetic application of top end "bleeder" type circuits. So, the circuit I posted doesn't have as much roll off. For better or worse.
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