L
Little Pigbacon
Guest
Re: Breaking in "guitar" electronics?
I don't think the output transformer requires a changing impedance. (Changing with time, I mean.) Does it require an impedance that changes with frequency? Probably not, but I suspect it may require higher impedances at higher frequencies -- which is what you get with series inductance.
Here's a graph I found that maps out the impedance of a typical driver:
Source: TGP. http://www.thegearpage.net/board/showpost.php?p=12546970&postcount=15
The impedance changes in that peak area because of "back EMF", which means the magnetic field created by the current through the voicecoil is contributing to the impedance in that frequency range by inducing a current in the coil that opposes the primary current. But this is the overriding scenario only in the range of the resonant frequency. Much below the resonant range, the DC resistance of the wire takes over; much above, the simple series inductance takes over.
I think the key to a well-behaved, happy amplifier is to make sure that it doesn't see anything scary in terms of impedances at any frequency. Some amplifiers can overheat at higher frequencies due to oscillation, which was the case with a particular amplifier design I encountered where the amplifier was intended to have -3dB points of 0 Hz and 3 MHz. You had to be very careful with input signals and everything on the output side to make sure it didn't run away.
I try to treat guitar amps pretty much the same way, particularly tube amps, as their circuit topology usually implies current source, and you don't want an amp trying to shove specific amounts of current into the primary side of a transformer when the secondary is open. The impedance of the speaker load is reflected (and scaled) back to the power tubes through the output transformer, and without the speaker load, the primary is mainly just coil resistance (and series inductance). It's like when you plug in a power supply that's AC-to-AC into the mains, without the product connected to the power supply. You often blow up the transformer or, if you're lucky, just pop the protection fuse.
Fair enough. "Inductive" here means that resistance is changing with frequency I assume, which is what a magnetic coil does. There is definitely a change in resistance here.
It is just that if the resistance changes with many Hz, I cannot think of a way to damage or otherwise change the output transformer. The reason why output transformer are damaged when run with no load is that they overheat and some of the winds melt. Changing the resistance pattern many times a second cannot build up heat.
Now, obviously you don't want to replace a 8 ohm impedance speaker with a D/C only resistor measuring 8 ohm D/C, because that will be a different resistance for A/C depending on frequency and the amp runs into the wrong resistance.
At the same time that illustrates why I am so skeptical about "artificial" loads damaging output transformers. The reason for me is that it is the speakers that constantly change resistance as you play. You play a full 1st fret F chord it has a different average resistance than if you play something high with the same volume. It is hard for me to imagine that the output transformer actually requires a changing resistance, and even if it does how do you ensure that your playing is the right pattern?
To me it looks far more likely that, if there is a difference at all beyond "no melting", that a constant resistance must be better.
I don't think the output transformer requires a changing impedance. (Changing with time, I mean.) Does it require an impedance that changes with frequency? Probably not, but I suspect it may require higher impedances at higher frequencies -- which is what you get with series inductance.
Here's a graph I found that maps out the impedance of a typical driver:
Source: TGP. http://www.thegearpage.net/board/showpost.php?p=12546970&postcount=15
The impedance changes in that peak area because of "back EMF", which means the magnetic field created by the current through the voicecoil is contributing to the impedance in that frequency range by inducing a current in the coil that opposes the primary current. But this is the overriding scenario only in the range of the resonant frequency. Much below the resonant range, the DC resistance of the wire takes over; much above, the simple series inductance takes over.
I think the key to a well-behaved, happy amplifier is to make sure that it doesn't see anything scary in terms of impedances at any frequency. Some amplifiers can overheat at higher frequencies due to oscillation, which was the case with a particular amplifier design I encountered where the amplifier was intended to have -3dB points of 0 Hz and 3 MHz. You had to be very careful with input signals and everything on the output side to make sure it didn't run away.
I try to treat guitar amps pretty much the same way, particularly tube amps, as their circuit topology usually implies current source, and you don't want an amp trying to shove specific amounts of current into the primary side of a transformer when the secondary is open. The impedance of the speaker load is reflected (and scaled) back to the power tubes through the output transformer, and without the speaker load, the primary is mainly just coil resistance (and series inductance). It's like when you plug in a power supply that's AC-to-AC into the mains, without the product connected to the power supply. You often blow up the transformer or, if you're lucky, just pop the protection fuse.