<font color='#000000'>Jon,
Somewhere along the line, theory and practice should find common ground. If this does not happen, then one disipline or the other is obviously at fault. In the case of a "far-end" zobel, it can have a profound effect on the signal at the speaker end, but will (usually) have a minor effect as regards the phase margin of the amplifier.
Where an inductor is used at the amp output, the effects are non-existent to the amplifier, since the cable is decoupled from the amp by the inductance at those frequencies.
You are right about the inductor/resistor BTW - it is not (strictly speaking) a "zobel network", so I suppose I had better stop referring to it as such to avoid any confusion
In the various simulations I have done so far, using a "lossy" transmission line (with R, L and C), the optimum value of the far end zobel resistance is equal to the line impedance. Since it is a rare speaker cable that has a characteristic impedance of 10 ohms, then that value is clearly not optimum as a "generic" fix. Although it reduces the amplitude of the primary reflection, it does not (and cannot) eliminate it. Instead, it just moves the peak somewhere else (typically to a much lower frequency)
Transmission line theory (and practice) indicates that this should be the case - a mismatch will
always cause reflections - only a perfectly matched transmission line is free of all reflected energy (standing waves).
Having looked at this more closely than before, I feel that there is good reason to use a far-end zobel, matched to the line impedance for RF. Doing so will make the speaker lead less likely to act as an antenna for stray RF fields, and minimising standing waves will ensure that a very wide bandwidth amp (without a series inductor) will not be affected. How many such amps are available? I honestly don't know, but for a 3 metre (10') cable, (Zo of 43 ohms) the first major reflection appears at around 5MHz - this is generally well outside the danger zone for most amps.
Predictably, longer cables will lower the frequency, but again, the use of 100nF and 10 ohms is ill advised unless the Zo of the cable is 10 ohms. Matching networks should
be matching networks, not "different mismatching" networks.
I am still gathering data on the characteristic impedance (and other parameters) for a selection of cables for my simulations, and hope to be able to publish some results shortly.</font>