In article , Iain M Churches
wrote:
"Trevor Wilson" wrote in message
...
The sales technician to whom I refer below tells me that
polytetrafluoroethylene (Teflon) capacitors are close to perfect with
sonic superiority, and have the lowest value of "tan d" (I am sure Jim
and Don will know what he is talking about:-) This is also what Andy
has discovered in his own listening tests.
FWIW from being involved in making lenses for use in the 30GHz - 1 THz
range then I'd say that the 'PTFE' and 'HDPE' families have low dielectric
loss values, and hence low tan delta values, up to frequencies like these.
However the loss does tend to scale with the frequency, so the losses of
many commonly-used dielectrics at audio frequencies should be quite low.
I am therefore somewhat doubtful that simple loss tangent values can
explain the claimed differences in audible performance. Precise models are
complicated, and we can consider the losses to have both 'shunt' and
'series' components. However a simple example can illustrate the reason for
my doubts.
I can't find any capacitor examples in the books I have at home, only
'optical' or dielectric propagation ones, so the following may be
incorrect. If so, someone let me know.
Lets assume a 1 microfarad cap with a nominal loss tangent of 1E-5 at
10kHz. IIRC This means that the in-phase (resistive) part of the impedance
is 1E-5 times less than the reactive part.
The nominal reactance of 1 microfarad cap at 10 kHz is 16 Ohms if I pressed
the right buttons on my calculator. :-)
This implies that if the loss is modelled with a shunt resistance we have a
shunt of 16 x 1E5 = 1.6 MOhms in parallel with the cap to represent the
loss tangent.
Alternatively, if we assume the loss tangent is a series resistance it will
have a value of (approx) 16 / 1E5 = less than 1 milli-Ohm.
Either way, I find it difficult to think that such small (linear) changes
in the total impedance have much effect. I suspect the resistive losses and
parasitics of the wiring would be more significant.
The reason for my question is that a local valve amp builder/component
salesman who uses Jensen caps, above all others has suggested that we
should build two identical µ-follower pre amps, one with Jensen and the
other with RS or Farnell standard components.
The interesting part here will be the 'identical' part... :-)
He says that the reason that Jensen seem to sound better is due to their
"dielectric absorption" factor. Music is made up of a series of
transients of pulses. If we apply such a pulse to a capacitor this is
equivalent to charging and discharging it, and that any voltage left on
the capacitor at the end of the pulse is distortion. He refers us to
Morgan Jones for further reading.
Afraid I don't regard a "pulses" description of musical waveforms like the
above to be very helpful. Real waveforms are rather more complicated so I'd
regard "pulses" as misleading here.
He is confident that a competent listening panel will pick and prefer
the amp with the Jensen caps, type for type. If not, some interesting
eating of hats will follow:-))
Mike G seems to have already done a similar test, with Jensen silver
foil caps in one channel of a power amplifier. His group picked out the
Jensen channel every time. I am not suggesting that these audible
differences only apply to Jensen. There are many other makers whose
products may well fall into the same category. Interesting.
The difficulty being that I haven't yet found either such reports - or the
attempts at specifying a physical mechanism - very plausible in the cases I
have seen so far.
Slainte,
Jim
--
Electronics
http://www.st-and.ac.uk/~www_pa/Scot...o/electron.htm
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Armstrong Audio
http://www.st-and.demon.co.uk/Audio/armstrong.html
Barbirolli Soc.
http://www.st-and.demon.co.uk/JBSoc/JBSoc.html