O
Omicron
Junior Audioholic
*sigh*You young ones crack me up..I used to think it fun playing with my food. Now it can be an annoyance..
Let me just defeat you with your own words then. This is what you wrote at the conclusion of our discussion about this same topic 2 years ago on the diyaudio forum:
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What is needed is to look at the system in segments, divided by an arbitrary line.
If one uses biwiring, select the segmentation to be between the amp and the cable plus loads.
Look at the amp which has A+B as an out, with it's dissipation of (a+b)2, while the load is split into two squares only.
Vs the monowire case, where one must set the segmentation AT THE branch juncture.
By segmenting at the juncture, the amp AND the wire both share the exact same power profile, while the load has the same one as always.
Where I was unable to consolidate the different power profiles was solely determined by where that segmentation occurs.
This view now squares entirely with what we were taught, and is consistent with what you have been stating..
I am now happy...and can easily reject the hypothesis that the selection of wiring scheme alters the signals via the 2ab component of a mixed signal power profile..perhaps in the near future, when I have my workshop back up, I will endeavor to do a test setup to confirm what we already understand..
Course, there are a few people who were on the railroad with me who were concerned with my sanity..did you realize that kinetic energy, gravometric potential, capacitor and inductor energy equations all share the same constructs as resistor dissipation?...(it is scary when I am given free time to dwell on this goop).
Kurt (and all others), it has been a distinct pleasure..thank you for your time and patience..
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Cheers, Kurt