TSSP: List Archives

From: Paul
Date: Fri, 15 Jun 2001 23:01:28 +0100
Subject: Re: [TSSP] Short Coil Experiments

Kurt wrote:

> the new measurements of the d=0.385m; h/d=1.15

Thanks. I've run these through the mill to get

 sk38b50: bare d=0.384m h/d=1.15 sr=0.79 turns=346 w/o mat
 f1    221.3kHz  230.1kHz +4.0%
 f3    506.5kHz  557.2kHz +10.0%
 f5    748.8kHz  882.5kHz +17.9%
 f7    831.0kHz 1222.5kHz +47.1%

without any correction for material dielectric.

(Kurt, the f7 measurement is suspicious - I'd expect something
 around 980 kHz.  I see you flagged it as questionable.)

The rising trend in errors is clear, and similar to what we have seen on
other coils, eg Finn's

 fh1: bare d=0.160m h/d=0.91 sr=0.86 turns=500 w/o mat
 f1    340.0kHz  361.8kHz +6.4%
 f3    725.0kHz  878.5kHz +21.2%
 f5   1100.0kHz 1355.9kHz +23.3%
 f7   1450.0kHz 1838.2kHz +26.8%

We've seen this pattern on other coils too, but thanks to these readings
we begin to see clearly that it is a small h/d thing.  Evidence
accumulates that the errors occur because we don't take account of the
material dielectric.  Finn's coil has 5.5mm of PVC (rel.perm = 3.4),
and Kurt's is 8mm of solid paper (rel.perm = 3.1).

If we take the material thickness as a percentage of the length, we get

 Kurt's: 0.8/44 = 1.8%
 Finn's: 0.55/14.5 = 3.8%

which we can use as an indication of the potential effect of the former.
I put in a rough correction for this, which came out with the right sort
of order of magnitude of change, which is encouraging.  It also improves
the results from larger h/d coils too, where the rising error trend is
still present, but less, eg Kurt's Sk-long coil:

 sk16b50: bare d=0.161m h/d=8.71 sr=0.85 turns=1976 w/o mat
 f1    152.3kHz  155.5kHz +2.1%
 f3    387.2kHz  385.8kHz -0.4%
 f5    564.2kHz  567.2kHz +0.5%
 f7    713.0kHz  725.8kHz +1.8%
 f9    850.0kHz  871.8kHz +2.6%
 f11   973.3kHz 1010.2kHz +3.8%

If we put in an approximate correction for the 3mm PVC, we get

 sk16b50: bare d=0.161m h/d=8.71 sr=0.85 turns=1976 matcor
 f1    152.3kHz  155.3kHz +1.9%
 f3    387.2kHz  382.4kHz -1.2%
 f5    564.2kHz  557.8kHz -1.1%
 f7    713.0kHz  708.4kHz -0.6%
 f9    850.0kHz  845.0kHz -0.6%
 f11   973.3kHz  972.9kHz -0.0%

which suggests that the correction is not quite enough. A similar
correction to Kurt's h/d=1.15 coil gives,

 sk38b50: bare d=0.384m h/d=1.15 sr=0.79 turns=346 matcor
 f1    221.3kHz  225.9kHz +2.1%
 f3    506.5kHz  525.4kHz +3.7%
 f5    748.8kHz  810.1kHz +8.2%
 f7    831.0kHz 1097.5kHz +32.1%

which, apart from the doubtful f7, shows a similar improvement.

The correction used counts as a fiddle factor, although the order of
magnitude is about right.  I'll have to do something a bit smarter, but
it means writing another laplace solver - about a days work. Fortunately
I only have to run it once in order to produce a suitable functional
approximation which can then be incorporated into the model.

Kurt, you also supplied results for Sk-5cm,

 sk5b503: bare d=0.051m h/d=8.03 sr=0.91 turns=934 w/o mat
 f1    979.7kHz 1030.8kHz +5.2%
 f3   2428.7kHz 2531.9kHz +4.3%
 f5   5300.0kHz 3707.7kHz -30.0%
 f7   6924.6kHz 4739.0kHz -31.6%
 f9   8643.1kHz 5694.6kHz -34.1%

Something a bit astray with f5 and above.  I get a better match if I
interpret the results as:

 sk5b503: bare d=0.051m h/d=8.03 sr=0.91 turns=934 w/o mat
 f1    979.7kHz 1030.8kHz +5.2%
 f3   2428.7kHz 2531.9kHz +4.3%
 f5             3707.7kHz
 f7             4739.0kHz
 f9   5300.0kHz 5694.6kHz +7.4%
 f11            6605.9kHz
 f13  6924.6kHz 7502.1kHz +8.3%
 f15            8384.8kHz
 f17  8643.1kHz 9272.9kHz +7.3%

and with material correction:

 sk5b503: bare d=0.051m h/d=8.03 sr=0.91 turns=934 matcor
 f1    979.7kHz 1027.3kHz +4.9%
 f3   2428.7kHz 2486.4kHz +2.4%
 f5             3585.5kHz
 f7             4519.3kHz
 f9   5300.0kHz 5363.7kHz +1.2%
 f11            6154.7kHz
 f13  6924.6kHz 6921.2kHz -0.0%
 f15            7666.8kHz
 f17  8643.1kHz 8410.0kHz -2.7%

Kurt, perhaps you can have a look for the missing resonances?

One last observation, concerning Q factors: The Q of Kurt's sk38b50
is very low, around 100, compared with a predicted Q of well over 500.
Is this the sonotube effect we see here.  My book on dielectric
properties gives the loss factor of paper/cardboard as 0.02, which is
abysmal.

I'll see if I can use a laplace solution to improve the material
correction, but so far it sure looks like it can account for the bulk
of the higher mode error.

Cheers,
--
Paul Nicholson,
Manchester, UK.
--


Maintainer Paul Nicholson, paul@abelian.demon.co.uk.