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Re: Wire length LC derivation,
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- Subject: Re: Wire length LC derivation,
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- Date: Sun, 13 Mar 2005 22:27:20 -0700
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Original poster: jdwarshui@xxxxxxxxx
Part 1
By Ampere, the inductance for a long air cored solenoid is:
L = (u Nsqrd A) / h (where h is the length of
the solenoid)
(where A is Area )
(where N is the number of
turns)
Since:
2 pi r N = wire length*
*actual wire length = sqrt ( (2pirN)sqrd + (h)sqrd )
but we disregard (h)sqrd as an insignificant term.
Then:
N = wire length / 2 pi r N
Substituting we get:
L = u ( wire length)sqrd / 4 pi h
By Maxwell:
u = 1 / Csqrd epsilon (Where C = 3x10 to 8 m/s)
Then:
L = (wire length)sqrd / (epsilon Csqrd 4 pi h )
Part 2
For sake of simplicity in the following description of LC we will use
the derived capacitance of an isolated sphere. This would be directly
applicable to a Tesla coil secondary.
From Gauss:
V = q/4 pi epsilon integral a to b for 1/ (r sqrd) dr
Since:
q = cap Volt
Then:
cap. = 4 pi epsilon (ab / b-a)
Since we have a single isolated plate, b approaches infinity
we get:
cap. = 4 pi epsilon R ( R is the radius of the sphere )
Now omega = 1/ sqrt (LC)
Substituting and canceling we get:
1/ (omega sqrd) = (wire length / 3x10 to 8 m/s)sqrd x ( R/h )
So:
[omega = (C/ wire length) x sqrt(h/R)
*R must of course be decreased to accommodate the self capacitance of
the coil.
Notice that the distance units cancelled for sqrt (h/R). Wire length
and the speed of light provide the units for 1/s
END.
Jared Dwarshuis, Lawrence Morris