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First designed for aerospace applications,
where performances must be outstanding, this cable is capable of conducting
hyper-frequencies. Its group delay characteristics make it a state-of-the art
cable when used in audio.
Its size may seem smallish to some, but was specially calculated for audio
applications. We claim this is one of the best existing cable to this day. Its
extremely tight manufacturing tolerance, the utmost quality of its components
and its anti-oxydation treating will make it a lasting choice.
Comparison with the best copper conductors reveals a greater subjective
linearity, a deeper low-end and an extremely natural treble. Its winding
geometry and its ultra-low resistance will allow you to use different lengths of
cable for your stereo channels without no sonic degradation.
About our
speaker cables and interconnects
Why
copper / silver ?
Metal is made of cristals linked together by a more or less conducting oxide
called the dielectric. The resistivity of copper and the resistivity of silver
are not highly different and should not, in theory, generate any significant
change in quality.
It is true, though, that silver oxide is a better electrical conductor than
copper. On the other hand, the influence of the dielectric is mainly significant
in high-frequencies. It is now known that, the higher the frequency, the more
the electrons will travel on the conductor’s surface.
We have consequently chosen a copper strand coated with silver. Both metals were
specially treated (LCOFC and anti-oxidation). This technology allows remarkable
sound, and reasonnable pricing.
To increase the silver conducting surface, and reduce capacitance problems, we
have adopted a winding geometry of nineteen 0,30 strands. Our cable is perfectly
reliable in a wide range of temperature, due to its molecular stability.
Why
Teflon ?
Electrons travelling in a wire generate resonances (who hasn’t heard
high-voltage wires «sing»?). These resonances are transmitted to the periphery
of the conductor, where they will disrupt the transmission of high-frequencies.
Teflon is able to absord important vibration, even when used in a thin layer. It
also «glues» to the conductor in a much more effective way than commonly used
PVC, preventing distortion to travel at the junction of the insulation.
To check this, try to bare a cable coated with both materials! Teflon will give
you a very hard time... Many manufacturers prefers to use PVC, though, because
Teflon is a costly insulator.
Why
Kapton ?
This material is a perfect insulator, able to dissipate without deformating very
high temperatures (it is also used for moving coil supports in some speakers).
Associated with an helical shielding, it also protects the signal travelling in
the cable from outside magnetic radiations.
Why
choosing 1,77 mm2 section ?
In high-fidelity and more generally in low-frequency, only low currents are
transported, so a large section is totally unnecessary (20 volts under 8 ohms
represent a 50 W power). The line resistance of the cable is the only data that
matters, and depends directly upon the metals’purity. Since our metals, both
copper and silver, are free from oxygen at 99, 5 %, the resistance of our cable
is 8 ohms/kilometer only.
Thus, when using 10 meters of cable, the damping factor of the amplifier will
always be above 33 for an impedance of 4 ohms, which is optimal.
How can you verify what we are asserting?
When soldering a common copper cable, caloric dissipation (hence, conduction) is
relatively low. You can hold the cable near the melting point without burning
yourself for some time. When repeating the same experience with our cable, heat
becomes immediately unbearable, forcing you to use pliers to hold the cable.
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Conductors |
| Core |
19 x 0,30 section 1,34
Tension 16 |
| Elements’ nominal diameter
|
1,77 |
| Strands’diameter |
0,15 |
| Composition
|
copper and silver
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| Line resistance |
0,008 ohm/M
|
|
Insulation |
| Conductors |
sheathed with filton F
(Kapton) |
| Shielding |
Helical
tinplated-copper |
| External sheath |
1st - Teflon layer / 2d
- PVC external covering |
| For use between |
- 90 ° to + 150 °
|
| Maximum voltage |
600 alternative volts |
| In accordance with AECME norms |
EN 2083, EN 2084 |
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