@williewonka
sorry you thought my post bombastic :-$ perhaps I get a bit carried away when fundamental laws are ignored.
The work is done by V pushing I through the load. If you measure a loudspeaker circuit, very little V is lost from either amplifier terminal to the speaker. Almost all V is across the load. Power is V x I. If the current were different in each leg of the cable, energy would either be gained or lost.
Apply a steady 1kHz 1V signal to a speaker. Regardless of where an ammeter is inserted in the circuit, the RMS current is the same.
In a DC circuit, V and I are in phase. In an AC circuit, V and I are not in phase if there is any L or C. Cable LRC change the phase and relative amplitude in combination with amplifier and loudspeaker LRC.
Phase angle is dependent on the difference between L reactance XL and C reactance XC, which vary with frequency. In cables like zip cord XL & XC may vary by a factor of 100 to 1. Some exotic cables XL & XC may vary by a billion to 1. XL can vary by a factor of 10,000 and more between zip cord and exotic cables. Exotic cables should endeavor to have less inductance, but some are worse than zip cord.
Asymmetric cables have a different L & C relative to parallel or woven and as such affect the current phase differently. These phase changes may be euphonious with some amplifier / loudspeaker combinations, not so much with others.
Some put sugar in coffee and prefer the 'sweetened' result.
One cannot, in absolute terms, say it is better [more accurate].
One can only say it is more accurate if one compares the source wave form to the resulting sound at your ear!
sorry you thought my post bombastic :-$ perhaps I get a bit carried away when fundamental laws are ignored.
the current (i.e. energy), or maybe even the voltage, in the neutral (i.e. minus) conductor cannot possibly be the same as the signal conductor.It cannot be otherwise. As you state, energy cannot be created or destroyed. It changes state in the load.
The work is done by V pushing I through the load. If you measure a loudspeaker circuit, very little V is lost from either amplifier terminal to the speaker. Almost all V is across the load. Power is V x I. If the current were different in each leg of the cable, energy would either be gained or lost.
Apply a steady 1kHz 1V signal to a speaker. Regardless of where an ammeter is inserted in the circuit, the RMS current is the same.
In a DC circuit, V and I are in phase. In an AC circuit, V and I are not in phase if there is any L or C. Cable LRC change the phase and relative amplitude in combination with amplifier and loudspeaker LRC.
Phase angle is dependent on the difference between L reactance XL and C reactance XC, which vary with frequency. In cables like zip cord XL & XC may vary by a factor of 100 to 1. Some exotic cables XL & XC may vary by a billion to 1. XL can vary by a factor of 10,000 and more between zip cord and exotic cables. Exotic cables should endeavor to have less inductance, but some are worse than zip cord.
Asymmetric cables have a different L & C relative to parallel or woven and as such affect the current phase differently. These phase changes may be euphonious with some amplifier / loudspeaker combinations, not so much with others.
Some put sugar in coffee and prefer the 'sweetened' result.
One cannot, in absolute terms, say it is better [more accurate].
One can only say it is more accurate if one compares the source wave form to the resulting sound at your ear!