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Re: Small TC experiments
Original poster: "by way of Terry Fritz <twftesla-at-uswest-dot-net>" <paul-at-abelian.demon.co.uk>
Ed Phillips <evp-at-pacbell-dot-net> wrote:
>>> ...If you keep the winding dimensions the same the inductance goes
>>> up as the square of the number of turns, while the resistance only
>>> goes up as the wire diameter. Net result is that the Q stays the
>>> same.
> This applies exactly to the ratio of the inductances of two coils
> of the same dimensions, ...
Of course. Apologies - I should have read your post more carefully.
> ... and also assumes that there is no insulation on the wires to
> reduce the winding factors as the wire diameter goes down. See
> Grover [71], p 117 and others on following pages. Of course, the
> inductance of a long coil of variable length doesn't go up as N^2.
> There's the little factor of Nagaoka's constant, etc.
> By the way, have you seen the expression for a very accurate
> closed-form calculation of Nagaoka which was in IEEE Proceedins a
> few years ago?
I have
'Inductance Formula for Single Layer Circular Coil'
HC Miller,
Proc IEEE, 1987, Vol 75 pt 2, pp256-7.
which uses a straightforward iteration of the elliptic integrals to
obtain both the bulk inductance and the mutual between filaments.
I haven't actually tried the method outlined so I don't know how it
compares with Grover - something else on my things-to-do list!
When it comes to calculating the Nagaoka inductance, I'm fond of
Lundin's formula, given in
'A Handbook Formula for the Inductance of a Single Layer Circular
Coil',
R. Lundin,
Proc IEEE, 1985, Volt 73, pp1428-9.
which presents a neat little formula for the inductance which is
claimed to be equivalent (to 6 figures) to interpolation over the 160
values of the original Nagaoka tables. I've found Lundin's formula to
be very reliable and easy to use.
Regards,
--
Paul Nicholson,
Manchester, UK.
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