jneutron said:
Farily confident that I did. I was very suprised by the relationships. ..I'm kinda busy here at the moment, but at lunch, I'll post all the equations and derivations, it's not very fast with the HTML code. That way, everyone else can look for errors on my part..
The prop speed is directly related to the mu and epsilon of the dielectric. Since we are talking about mu =1 here, the prop speed is only related to the epsilon of the insulation for coaxial structures.
Cheers, John
Ok..the eq's. D.C. is epsilon, the dielectric coefficient..
First, the capacitance of a coaxial line..
C = <sup>(2 * pi * D.C.)</sup>/<sub>Ln(<sup>R<sub>o</sub></sup>/<sub>R<sub>i</sub></sub>)</sub>
Next, the inductance of a coaxial line..
L = (<sup>mu</sup>/<sub>2*pi</sub>) * Ln(<sup>R<sub>o</sub></sup>/<sub>R<sub>i</sub></sub>)
Re-arrange both equations, with Ln(<sup>R<sub>o</sub></sup>/<sub>R<sub>i</sub></sub>) on one side:
Capacitance:
Ln(<sup>R<sub>o</sub></sup>/<sub>R<sub>i</sub></sub>) = <sup>(2 * pi * D.C.)</sup>/<sub>C</sub>
Inductance: set mu =1, as the dielectric is non magnetic:
Ln(<sup>R<sub>o</sub></sup>/<sub>R<sub>i</sub></sub>) = (L * 2*pi)
Note: both equations equal the Ln ratio, so equate them..
<sup>(2 * pi * D.C.)</sup>/<sub>C</sub> = (L * 2*pi)
The 2 * pi's cancel:
<sup>(D.C.)</sup>/<sub>C</sub> = L
Bring C to the right:
D.C. = LC
This means that for a specific insulation type, the product of L and C will be a constant. Note that no where within that result, is the specific radii of the inner conductor, or the outer braid radii..they were cancelled out at the beginning of the analysis.
Weird, ain't it??
Note that up to now, I have been using L * C = D.C. *1034. It is interesting, in that I have been using nHenries for inductance, and pf for capacitance...If I used pH for inductance, this would have been L * C = 1.034 * D.C.
I believe, though have not tried yet, to find out if that 3.4% error is a result of truncation or rounding from the data I used for my initial analysis. (ya always gotta check your sources, guys...lots of garbage out there on the web that is just totally inaccurate..
OH, also...
Impedance Z = sqr(<sup>L</sup>/<sub>C</sub>)
And
V <sub>(fraction of lightspeed) </sub> = <sup>1</sup>/<sub>sqr(LC)</sub>
also stated as:
V <sub>(fraction of lightspeed) </sub> = <sup>1</sup>/<sub>sqr(D.C.)</sub>
What is significant, and the entity that Jr didn't understand, is that when a cable is measured, giving an L and C, the product of those gives the EFFECTIVE DC, which provides the boundary line for that construction geometry, and the velocity of propagation...
With the LC graph of D.C. and the one of velocity, any cable measured can be quantified as to the utilization of the geometry.. In other words, how close it comes to coaxial cable when it comes to containing the magnetic and electric fields..
Everybody: Please check my math....I've been wrong before, (just ask my ex)
Oh well...back to the winding machine...
Cheers, John..
Oh man, writing eq's with html is a PITA...hope I didn't have any typo's..