It looks like you're new here. If you want to get involved, click one of these buttons!
Subscribe to our Patreon, and get image uploads with no ads on the site!
Base theme by DesignModo & ported to Powered by Vanilla by Chris Ireland, modified by the "theFB" team.
Comments
"Take these three items, some WD-40, a vise grip, and a roll of duct tape. Any man worth his salt can fix almost any problem with this stuff alone." - Walt Kowalski
"Only two things are infinite - the universe, and human stupidity. And I'm not sure about the universe." - Albert Einstein
"Take these three items, some WD-40, a vise grip, and a roll of duct tape. Any man worth his salt can fix almost any problem with this stuff alone." - Walt Kowalski
"Only two things are infinite - the universe, and human stupidity. And I'm not sure about the universe." - Albert Einstein
The main caveats with the amp IMO are:
I've done a similar experiment to ICBM with home built 18 Watters, one using 6V6's and the other EL84's, the difference is very subtle, it's the circuit that shapes the sound not the valves, everything matters though, but not as much as many people think
ICBM's what makes an amp list is pertty accurate, personally I'd change it a little bit as follows:
Circuit design
- preamp topology
- power amp topology
Speakers
OP Transformer type
Component types
Cabinet design
Valve type
Cabinet material
Circuit layout
Wiring dress
Valve brand
Grille cloth
Cabinet covering
Chassis material
Negative feedback is where a small part of the output signal of a stage is fed back into the input of it, out of phase, so it counteracts the amplification to some extent. This is useful because it helps to smooth out non-linearity in the stage, so although you get less gain, you get a cleaner sound, and wider and more even frequency response. It also reduces the output impedance of the stage and increases its damping factor so it becomes less dependent on the load.
In most amps it's done on the power stage, so the loss of gain is not very important anyway, but you get closer to a 'perfect' output stage. (As you may have guessed, this comes from hi-fi design originally.) Usually the signal is fed back in at the phase inverter.
The result is a cleaner, clearer, 'bigger' sound but also more hi-fi, ie less 'characterful' in some ways. When the power stage distorts, it gets more complicated because the NFB is abruptly cut off at the point of distortion, so the transition to distortion becomes sharper and the distortion 'harder' in character. A perfect example is the difference between a Vox AC30 (no NFB) and a Marshall Bluesbreaker (heavy NFB). Both amps are fairly similar-sounding clean (not exactly obviously), but the AC30 has a very bouncy, compressed overdrive where the Marshall is much tighter and crunchier.
Usually a presence control removes high frequencies from the NFB loop, which takes away some of the damping at the top end and makes the highs more dynamic and lively, which makes the amp more 'present' in a mix, hence the name. A resonance control is the same but works on the low-end, or sometimes just on the whole amount of the NFB - it makes the amp sound looser or more resonant - at the expense of making it much more speaker-sensitive. A great example is the Modern High-Gain mode on the Mesa Dual Rectifier, which turns off the NFB entirely just in that mode - that's what gives the huge boomy 'Recto' tone, but makes it very fussy about using the right cabinet. (The presence control on that channel works in the preamp instead.)
"Take these three items, some WD-40, a vise grip, and a roll of duct tape. Any man worth his salt can fix almost any problem with this stuff alone." - Walt Kowalski
"Only two things are infinite - the universe, and human stupidity. And I'm not sure about the universe." - Albert Einstein
The MJW Orion and Electra use separate cathode resistors (when cathode biased), but I'll forgive you for not being aware of those!
I'm using it as a way of reducing power output, ideally without altering the tone too much. There is a small change to the tone and feel of the amp, but it's hard to say how much of that is because of the power reduction and how much the change of bias method.
In an amp with a shared cathode resistor then a valve failure means the remaining working valves become biased hotter, which especially dangerous in amps with over dissipating EL84s.
In a true class A amp driven below clipping the sum of the current draw through each side of the power stage is constant, and thus the voltage across a common cathode resistor will be constant. In practice there will always be a slight variation and thus a cathode bypass cap is used to shunt ac current to ground.
In a class AB amp (ie virtually all "class A" guitar amps), when the current draw from the power supply is NOT constant as the amp is driven harder. The cathode bypass cap does shunt some of this extra current to ground but when the amp is driven hard the extra current causes the cathode bypass cap to charge up increasing the cathode voltage, ie the amp becomes biased colder as it is driven harder.
This is actually stated on the JMI AC30 schematic, which indicates a power valve cathode voltage of "12.5V AT 30V, QUIESCENT 10V", which of course indicates class AB operation........
As most of the current flow (if not all) with be from the positively driven side, the current through one side of the push pull pair affects the bias of the other side, and, in my view, is part of the cathode bias sound.
At best this will increase crossover distortion, and at worst will cause blocking distortion where amp is driven into cut off.
The amp will only return to "correct" bias conditions once the cathode resistor can discharge, and this will depend on the value of the capacitor and the impedance it sees to ground.
In a fixed bias amp, the bias is set by a negative voltage applied to the grids of the power valves, and this will vary very little, if at all, with level of power valve drive.
Using separate cathode resistors for each valve to bias the output stage, then the current draw on one side of the push pull pairing with not affect the biasing of the other side (in fact the other side will be biased hotter as the cathode bypass cap discharges). Thus the relationship between the biasing and drive levels with be more akin to fixed bias, and the opposite of cathode bias with a common cathode resistor.
For those of you how have managed to read this far, I haven't mentioned grid conduction; suffice to say this phenomenon exacerbates the differences between bias methods; however I think that this post is long enough already!
The use of separate cathode resistors seems to have been popularized by Mullard in their application notes, although I don't know if they were the first, and my guess is that is this was either a tacit emission of class AB operation, or a method of temporary overloads more benign.
Regardless of the sonic properties of cathode/fixed biasing, If you want to incorporate bias balance with pure cathode biasing, then you will need a fairly hefty pot to cope with the bias current if you what the amp to be reliable, so a small element of fixed bias is a sensible approach.
Also, adjusting a cathode bias pot would create a ton of noise, and you can imagine the number of communications you would have about this!
"Take these three items, some WD-40, a vise grip, and a roll of duct tape. Any man worth his salt can fix almost any problem with this stuff alone." - Walt Kowalski
"Only two things are infinite - the universe, and human stupidity. And I'm not sure about the universe." - Albert Einstein