Thanks Roly!
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Show posts MenuQuoteI'd encourage you to run through this again setting the Collector load 1k to 10kThanks Roly, and I did just that. If interested, please see attachment. Hopefully I have it right! I had to post it as a .pdf so it spreads over three pages but it still quite readable.
Quote6mA through 1k is 6 volts, so the Collector voltage will drop by 1 volt.I'm assuming we're using variables to understand the workings of a transistor and wouldn't really be applicable as I remember that we wanted a max. 5 volts at the collector, half the 10 v supply so we could have a clean audio amplification stage.
Quote{I had a funny feeling when I wrote that ... you ever consider doing an electronics course?Roly so here's my story: fifteen years ago I completed an electronics certificate at the college level, had ideas of getting into the audio repair business, but kids, mortgage and other pressures put that on the back burner, way back! so now, with adult kids and at age 53 I'm gradually dusting off my knowledge and asking many questions. There are definitely holes in my knowledge and it's amazing what you can forget in fifteen years--usually the small connecting details/equations/theory but it's coming back and I pretty much spend a couple of hours a day with my head in this stuff with an eye to start up a part-time repair business down the road. I'm having a blast and loving it!
QuoteInstead of looking to simulate circuits, consider buying a few cheap transistors and some cheap resistors and a few caps, and actually making little circuits. Then a basic voltmeter can take readings in the circuit.Enzo, that makes total sense. So should I be thinking about getting a DC Power Supply? any recommendations in terms of max current/voltage?
Quotebut when we want to operate the transistor in grounded Emitter mode so we can get some voltage gain on the Collector,Sorry, couldn't resist another question. Firstly, excellent description and I understand most of it! Great stuff and thanks Roly! So, as for the quote above, my mind was going along beautifully with your description until I read the bit about the voltage gain on the Collector if we grounded the emitter. Could you elaborate on how we achieve voltage gain on the collector? Is it because more current is flowing through the collector due to the removal of the emitter resistor and therefore the increased current multiplied by the Collector's internal resistance creates a greater voltage? That's what messes me up about Transistors-- I understand the base current loop creating current flow from Collector to Emitter, like a valve letting more water through, and then I think I've got this stuff, but when we start talking from Emitter to Collector I start thinking about holes filling valence shells missing electrons and conventional current. With transistors should we be thinking neg to pos/conventional current at the same time? Or should we always think neg to positive--N type material to P type material-- just to keep our heads on straight? Should we not overly concern ourselves with current flow from emitter to collector? Thanks!
Quote... I have made use of this characteristic to fit a linear scale wattmeter to my dummy load. It's a bridge rectifier, but the voltage is scaled down by resistances so that it operates over the early part of its conduction curve, and the result is a current of 0-1mA for 0-100W in 8 ohms (calibrated to be exact at 50 watts, leaving an error of about 5% at 10 and 90 watts.}Sounds great, I'd like to see a picture if you have one.
QuoteI've mentioned the internal series resistance into the Base, but there is an effective series resistance with every terminal, and the one in the Emitter is a particular trap because it appears not only in series with the controlled main C-E current flow, but also in series with the controlling Base-Emitter flow (and thus results in unwanted local negative feedback within the device). {This is normally called something like r'e, emitter resistance, where the apostrophe implies an internal property.}
QuoteSo we put in some bias between the bases so that both transistors are conducting just a little bit, idle current, and the transition from one transistor conducting to the other is much smoother (and much better sounding).So this would explain the presence of DC voltages at the bases of TR6 and TR5, so that both transistors are conducting and therefore we eliminate crossover distortion:
Quotethe voltage across the EB junction may stay the same - remember it is a "diode", not a resistor - changing current through that junction controls current through EC. SO while you play, look at the voltage on the collector of that transistor.I tried that: referenced to ground, on collector of TR6 I get 36.7vdc at idle. At full volume, guitar playing, 35.8vdc. So, from this info, it looks like the pos. signal excursion has pulled down the voltage a little, correct?
QuoteAt idle both upper and lower output transistor "clutches" are just conducting thanks to the idle bias setting. The half-rail is at ground potential, and the bias network is pushing the Bases just far enough apart to let through a dribble of current.
QuoteNow, just pretending for a moment that this circuit doesn't have the NFB blooper and in fact has proper NFB. What would the output DC offset be in this amp?
{hint: the base of the first transistor is tied to ground via the 10k, so applying very basic transistor knowledge, the voltage on its emitter must be... and therefore...?}
QuoteThe DC point is set by the 10k to ground on the "+" input, so it basically "follows" ground for DC.Could you possibly re-explain this, not quite sure how that works.
QuoteFor AC signals where the reactance (or AC resistance), Xc, of the cap is low then the ratio of the feedback resistors sets the AC gain.
QuoteFeedback in s.s. amps is a bit of a trick because it is both DC and AC.So what is blocking DC from entering the speaker? I see C6 which goes to ground, does that mean that it is easier for DC to go to ground then the speaker? I expected to see a DC blocking coupling cap between OT's and speaker...hmmm
QuoteThe attenuation of Rf and Rs at AC is;Roly, looks like you are using a voltage divider equation, but not sure how you get V1,/V2 also equal to 0.04347826? Could you detail this a little more if possible?
Rs / Rf+Rs
1 / (1+22) = 0.04347826 times
dB = 20 log10(V1/V2)
20 * log10(0.04347826) = -27.23455689dB
QuoteThanks Roly for the details, what you're saying about the feedback circuit reinforcing makes sense. But what exactly is happening when you say:
This in turn will cause it to pull its collector more positive, and since this is also the bias point it will turn on the clutch of upper transistors, and turn off the lower clutch, so the output half rail will be pulled positive.
Now this positive-going signal is taken back to the base of the second transistor, but it has just had its emitter pulled negative, so this positive-going feedback signal will actually try and turn on the second transistor harder, and the VAS, and the output clutch.
Quoteand since this is also the bias point it will turn on the clutch of upper transistors, and turn off the lower clutchHow is the lower clutch turned off? Is it all about pos relative to negative, depending on the situation? Upper Clutch being more positive, lower clutch less positive and closer to a value less than turn on voltage? Thanks. :tu: