Mudcat said:
It was oriface derived, but again, as in the past, your charts back up my guesses.
Oriface??? as opposed to orifice?
(tag, you're it)
Mudcat said:
That whistling sound you just heard was a shot across the bow.
He he...ya killin me...
Mudcat said:
I make another SWAG that I'll be in for it now.)
"S" being scientific??
Mudcat said:
And no you are correct, I totally forgot about the effective dielectric coefficient.
Umm, ya got me there...I wasn't aware of saying anything that was "correct", vs something you said that wasn't...and in the context here, I use "effective" DC as what the dc appears to be, not "relative" DC.
What was really neat in my derivations, was that it's possible to determine the effectiveness of the geometry of the wire construct by measuring the L and C, and deriving the effective DC from those two numbers..If you use teflon as the Dielectric, and get an effective dc of 6.25, for example, then you know the geometry is not as good as it can be, the design is not very efficient.. 100% efficient geometries will have the LC point fall directly on the DC curve on the graph.
(oh, btw..the actual equation is L*C=(mu times epsilon)/c<sup>2</sup>
mu being relative magnetic permeability
epsilon being relative dielectric constant
C being speed of light..
My gut feeling is that the higher the prop speed, the better the wire will be for speaker apps (nuttin to back this feeling with at this time..but I note that prop speed is related to L*C product.) Also, the closer to load characteristic impedance, the better...again, a WAG on my part..just a feeling..
I've resisted working on the metrics you are designing for the relative merit of wires, because I'm wrestling with these gut feelings theoretically..
I'm currently workin on the dipole soundfield technology, and how it relates to the virtual image construct..really fertile ground...fun to wrestle with. and, methinks, totally applicable to deriving how virtual imaging is susceptible to variations in time relationships..
Cheers, John