| Silversmith
Audio
Silver
Interconnect
and
Speaker
Cable |
|
|
Mike
Silverton |
|
11
March 2002 |
Specifications
8-foot
Silversmith Silver
Speaker Cable,
$2950.
4.5-foot balanced
(XLR-terminated)
Silversmith Silver
Interconnect,
$1650.
Address
Silversmith Audio,
4946 Pacifica
Drive,
San Diego CA 92109
Phone 858 272 6375
Website: www.silversmithaudio.com
Email: info@silversmithaudio.com
In
the matter of
audiophile cabling
- there being a
pasta factory's
abbondanza - I
attend to those
cognoscenti I
trust. Harry
Pearson and Scot
Markwell's
enthusiasm for
Nordost's Valhalla
line proved itself
in my listening
room. Another
knowledgeable
enthusiast, Kevin
Tellekamp, the man
behind Silent
Running Audio, put
me on to Jeffrey
Smith's
Silversmith Audio.
Kevin, whose
superb isolation
platforms sit
under my Mark
Levinson hardware,
doesn't mince
words: Smith's
wires trounce the
lot. We'll get to
my opinion soon
enough. Meanwhile,
Silversmith's
eponym has sent me
several emails
from which I'll
quote at length.
This remains a
controversial
topic (as does so
much in high-end
audio). A
practitioner's
assertions are
bound to fascinate
the engaged
reader. My
occasional
italicized asides
appear within
brackets.
"Briefly,
my design centers
around a single,
ultra-thin,
solid-core ribbon
per polarity (one
each for positive
and negative
runs). The ribbons
[three-quarter-inch-wide
conductors]
for the speaker
cables are
self-contained in
their own jacket
system, which uses
extremely
thin-walled Teflon
tubes to protect
them as well as
maintain a
primarily air
dielectric. There
is so little solid
material in the
speaker and
interconnect
cables that you
can actually see
through them. In
the interconnect,
each ribbon is
also enclosed in
an extremely
thin-walled Teflon
tube; the
ribbon/tube runs
are then encased
by the outer
thin-walled tube
that gives the
interconnect its
flexibility [the
most flexible I've
ever handled].
"One
of the first
things you'll have
noticed about the
speaker cable is
its lack of a
traditional
connector. In
notching the [protruding]
ribbon in the
shape of a spade
lug, I can avoid
the signal damage
a connector
causes. A word of
caution: while the
[notched]
ribbon is
surprisingly
resilient, it is
obviously more
fragile than a
traditional
connector and
should be treated
with care. Also,
its width can
cause connection
difficulties with
narrowly spaced
binding posts. I
recommend using
the Velcro straps
that I enclose
with all cables,
to keep the
speaker cables
together, wide
edge to wide edge,
and enter the
binding posts from
opposing
directions. This
will keep the
ribbons from
touching and
shorting out. [A
necessity. My
speakers' binding
posts are too
close to
accommodate the
wide ribbons in
any other way.]
With regard to my
single-ended IC,
my concern over
connector-related
degradation led to
my choice of the
Bullet Plug by
Eichmann
Technologies out
of Australia.
Instead of the
error-inducing,
massive metal
construction that
seems to define
other RCA
connectors, the
Bullet Plug is an
all-plastic design
with small, hollow
and thin-walled
pins. The sonic
improvement this
connector affords
is
astounding."
Smith
offers two lines,
Silver (here
discussed) and
Palladium. The
latter takes its
name from that of
a drop-dead
expensive metal
that, in Smith's
words, "will
not oxidize or
otherwise tarnish
and therefore will
not degrade
sonically over its
lifetime." I
expect to receive
a review pair of
the Palladium IC's
in about a month.
Smith also
produces a
Palladium speaker
cable but, as the
cost of the metal
is so prohibitive,
he's yet to reward
himself with a
set. A review pair
lies somewhere
over my rainbow.
Speaking
of lifetimes,
several ago, I ran
two Crown Macro
Reference amps as
a mono pair. For
the best bass
reproduction, The
Crown manual
suggested speaker
cables thick as a
linebacker's neck.
I mention this
only to point up
an absurd
disparity. When
Smith says there's
not much to his
cables content
wise, he's not
just whistling
three-voice
fugues. Should
that put us off?
Only if we equate
mass with quality,
in which case,
I've these
exquisite concrete
pavers I'm willing
to sacrifice….
As a technically
unlettered
listener, I can
only report that
the heft issue
seems irrelevant
to what I'm
hearing my
system's low end
doing.
In
answer to a
question about
dielectric
constants (a
conductor's
proximity to
operating within a
vacuum, i.e., the
ideal
environment),
Smith has this to
say:
"I
have not taken
measurements, but
the dielectric
constant should be
close to 1 [the
ideal].
Similarly, I have
not measured
actual LRC
(inductance,
resistance,
capacitance)
values, though,
given the geometry
of the ribbons,
those can easily
be derived and are
very low. Still,
they have nothing
to do with the
sound of a cable.
[Bravo! If only
the
pocket-protector
types would sit
down and listen!]
In any event,
because my
conductors are
free floating and
can change their
relative position,
those values
fluctuate
slightly.
"I've
heard your comment
about a very
different sort of
sound from quite a
number of people.
[I had offered
Jeff some
preliminary
impressions.]
Solid dielectrics,
multiple strands,
thick wire, and
massive connectors
are all causes of
signal alteration,
i.e., time
smearing, tonal
shift, loss of
resolution,
dynamics,
transparency, etc.
I did not design
my cables to be
the best sounding
on the market.
Doing so implies
using one's own
amplification,
speakers and
source material to
subjectively
determine what
sounds best to
one's own ears.
Using established
engineering
principles
concerning
electromagnetics,
transmission lines
and wave
propagation, I
simply designed my
cables to do the
least possible
damage to the
electrical
waveform. I worked
out the design
entirely 'on the
drawing board.'
Only then did I
actually build and
listen to the
cables to ensure
that the cosmetic
choices I made did
not cause any
sonic degradation.
Few people have
ever experienced a
low-error cable,
and that is the
reason I
frequently hear
observations such
as yours.
"Unfortunately,
this low-error
quality can be a
double-edged
sword. Some
systems need a
tone control,
specifically a
resolution-restricting
cable, to achieve
a sound to the
listener's liking
or to cover a
system's flaws.
For better or
worse, my cables
reveal naked
truths, those of a
system as well as
recordings. Also,
while my Silver
and Palladium
cables are far
from the worlds
most expensive,
they are somewhat
pricey. I make
them entirely by
hand and utilize
the finest
materials
available. The
review samples you
received represent
about a day's
efforts at the
workbench. These
designs cannot be
extruded or
otherwise
mass-produced. The
Silver line is
priced low enough
so that most
audiophiles can,
over time, pick up
a cable or two.
Adding just a
single set of
interconnects can
really transform a
system. Be
careful! Several
of my customers
have reported
sleep
deprivation."
That
last sentence
could stand as a
model for the kind
of exuberance
niche-market
providers bring to
their disciplines.
What sets me apart
from Jeff Smith,
and by extension,
you, the concerned
reader, is needful
diffidence. As a
breed, we remain
alert to the
possibility of
improvement but
are wary of wackos
and frauds. Our
shared passion
emerged a good
half-century ago
as high fidelity.
Over the decades,
designer-manufacturers
have made claims
that would bring a
blush to Baron
Munchausen's cheek
and, in certain
cases, an end to
the physical
universe as we
know it. On the
other hand,
seasoned listeners
are well aware of
those minute and
gross differences
various audio
components bring
to the mix. That's
where the
observationalist,
a.k.a.
subjectivist,
audio reporter
comes in. He's
very much like a
medium. Rather
than the spirit
world, he conveys
his impressions of
what emerges from
a realm not far
removed, the
ghostly sound
field. But before
I do my part,
let's let Jeff
Smith hold forth a
little longer.
This is, as I say,
a hot-button
subject, and we
need to learn as
much about it as
we can.
As
these Silversmith
designs are far
from conventional,
it seemed prudent
to ask Jeff about
cables as
contributors to
amplifier
instability. While
my Mark Levinson
amps are probably
as stable as they
come, some designs
operate closer to
the edge and are
therefore a cause
for concern.
"It's
true that speaker
cables can cause
certain amps to
oscillate. The
culprit is high
capacitance. The
primary factors
that determine
capacitance are
surface area,
distance between
conductors, and
the dielectric.
Obviously, a wide
ribbon like mine
has quite a bit of
surface area, but
the distance
between the
conductors is
extreme, so the
resulting
capacitance is
lower than that of
most cables."
Kevin
Tellekamp
mentioned the
curious fact of a
military network
within high-end
audio.
"Yes,
my background is
military. I am a
Naval officer,
having graduated
from the US Naval
Academy with a
degree in
engineering, and
am now in the
Naval Reserves
after eight years
of active duty.
During my last
assignment, a
shore tour as an
instructor at a
combat training
facility here in
San Diego, I began
working part-time
at a high-end
audio shop. One of
my co-workers, a
dedicated DIYer,
got me excited
about building my
own speakers.
Having access to
the Navy's wood
hobby shop and
some woodworking
skills, I thought
it sounded like
fun. After
building the
speakers and
wanting to get the
best sound
possible out of
them, the question
of how to wire
them came up. I
conducted some
research and,
after discovering
quite a few things
impacting cable
design that most
engineers,
surprisingly,
aren't taught, I
realized that
there is only one
way to construct
an audio cable
that does not act
as a tone control.
After fabricating
a prototype, I
knew I was on to
something special
and decided to
pursue it. Ralph
Dodson, the man
behind the Dodson
Audio DAC (you
have to hear it if
you have not
already), used to
frequent the store
and participated
in a few listening
tests. Ralph was
impressed and
called Lars
Fredell of Ultimate
Audio to tell
him about my
cables. This all
took place before
I was officially a
company. I shipped
some cables off to
Lars to listen to
in the summer of
1999 and, during
his evaluation, a
few people visited
and heard them as
well, including
Kevin Tellekamp
and Vladimir
Shushurin of Lamm.
In what seemed a
whirlwind, I
officially started
Silversmith Audio
on the first of
January, 2000 and,
four days later,
exhibited at CES
with Lamm/Nearfield
Acoustics,
Eggleston/Wadia,
and Lamm/Verity
Audio/Bybee. I
could not have
asked for a better
start."
And
now, despite my
best efforts to
remain the
dignified,
distanced skeptic,
I revert to the
drooling fool we
audiophiles
becomes at moments
such as this.
Until I hear
Smith's Palladium
IC, these Silver
ICs and speaker
cables are
probably going to
be my Products of
the Year. Never
has this system
sounded so
musically right.
Great, yes, but
never so right.
Prior to
Silversmith, I'd
achieved a
totality fairly
oozing resolution,
a beautifully
arrayed stereo
image, precise
dynamics, timbral
truth; all those
sonic lovelies we
strive to achieve.
I thought I'd
climbed to the top
of the hill. As
always, there's a
tad more terrain
to ascend. In the
language of
Wheezing Moose,
the penultimate
Mohigan, these
Silversmith cables
bring to the event
that certain
jenny-say-kwa: in
audiobabble, a
heightened sense
of coherence,
space,
dimensionality,
and harmonic
texture, and the
picture holds
together, no
matter how large
the force or loud.
For
my part, hardware
reports convert to
crashing bores
when the reporter
begins detailing
the recordings
he's played.
Suffice that I
listened to many.
As a curiosity,
indeed, as perhaps
the most
interesting aspect
of these sessions,
the sense my
Valhalla cables
convey of
extraordinary
resolution and
transparency these
Silversmith cables
in no way
diminish. Far from
it! With
Silversmith, the
recording takes
precedence. In
making direct
comparisons
between the
Silversmith Silver
IC and speaker
cable and the
Valhallas, the
latter remain (to
say it again)
bears for
resolution,
transparency,
soundstage and
dynamic finesse.
The Silversmith
Silver cables' way
with musical
texture, the
feeling they
convey of a
lifelike,
extraordinarily
dimensioned space
proved by no small
degree the more
satisfying
experience. With
Silversmith, one's
consciousness of
transparency and
resolution defers
to one's immersion
in the recording.
To
return to
neck-thick cabling
for maximum bass
response and the
physics governing
such matters, I'm
baffled. Together,
these
insubstantial
Silversmith ICs
and speaker cables
permit a supremely
rich low end,
along with a
midrange - I was
about to write
"money can't
buy" until I
thought about that
for a moment. An
early perception
of low-end
pudginess has
given way to utter
satisfaction as
the cables
matured. Smith
thinks they're 95%
ready out of their
black satin
pouches. I'll only
add that it takes
perhaps a dozen
hours for them to
perform spot on. I
believe I've found
the answer to the
question,
"Where's the
beef?"
The
Silversmith Silver
ICs and speaker
cables operate in
what sounds to me
like celestial
synergy. I
hesitate to guess
what it is about
the speaker cable
that makes it
sound so
absolutely right.
Its innovative
termination, the
notched ribbon
conductor? The
foil-like ribbon
that just about
floats in air? I
only know that I
love what I'm
hearing. Let's end
with Smith's
thoughts on the
Great Cable Flap:
"As
an engineer, I was
taught that
electrical energy
flows up the
positive conductor
and back down the
negative conductor
in a loop, like
water in a pipe.
This analogy is
simple and makes
circuit analysis
easy. Inductance,
capacitance, and
resistance (LRC)
are the only
factors
considered. This
is the primary
reason some
engineers say that
wires cannot
possibly affect
sound. Based
solely upon LRC
parameters, that
would be the
correct assertion.
However, these
engineers were
either not taught
or forgot the
assumptions that
allow them to use
the
water-in-a-pipe
analogy.
Dielectric factors
such as absorption
and polarization
are very small and
do not affect
circuit analysis;
self-inductance
and mutual
inductance are
similarly small
and can be
ignored, along
with the
assumption that
skin effects are
negligible. In
normal, low
frequency circuit
analysis, these
assumptions can
pass for valid.
However, in
applications that
involve human
hearing, they
won't fly.
"To
understand how
these affects
impact our
perceptions, and
how to eliminate
them, one must
understand what
really happens in
the flow of
electrical energy.
The water-in-a
pipe-analogy is
not entirely
accurate. Instead
of traveling in
the conductors,
energy flows between
the conductors, in
the dielectric, as
an electromagnetic
wave. As the
electromagnetic
wave passes
through the
dielectric, some
of its energy is
momentarily stored
and then released;
some is actually
absorbed and lost.
These polarization
and absorption
effects are
non-linear. They
occur at varying
rates in different
frequency ranges
and are material
dependent. We
perceive the
results as, among
other things,
coloration. Each
solid (and even
liquid) dielectric
has its own sound.
I associate the
Teflon sound with
a nasal quality in
the male vocal
range. Teflon is
actually a very
poor choice for
the primary
dielectric in an
audio cable.
However, of all
the solid
materials, it is
the least
objectionable. Air
is polarized at a
much higher
frequency and its
energy storage and
loss are far, far
less than that of
any solid. Just
think about the
difference in the
number of
atoms/molecules in
a given volume
between a gas and
a solid. We cannot
hear the
coloration a
gaseous dielectric
contributes.
"The
propagation speed,
the rate at which
the
electromagnetic
wave travels down
the cable, is also
material-dependent
and is typically a
large percentage
of the speed of
light. Does the
actual value of
the propagation
speed have any
bearing on the
sound of a cable?
Can a person hear
the difference
between a
one-nanosecond and
a two-nanosecond
arrival time of
sound to their
ear? Obviously,
the answer is no.
Nonetheless,
propagation speed
is important in
that it is an
indication of the
dielectric's
quality. A purely
gaseous dielectric
will have a
greater than 99%
speed-of-light
propagation.
Lesser-quality
dielectrics will
be much slower.
"Where
propagation speed
does have a
dramatic effect is
in the nearly
universally
misunderstood
concept of skin
effect. Contrary
to popular belief,
the higher
frequencies do not
ride in the outer
regions of the
conductors. Once
again, energy is
conveyed between
the conductors,
not in them. As
the
electromagnetic
wave travels along
a cable, however,
it will penetrate
the conductors. As
it penetrates, the
wave is rapidly
attenuated, with
the higher
frequencies
undergoing more
rapid attenuation
than the lower
frequencies as
they journey
towards the
conductor's
center. If we look
at a cross section
of a round
conductor, this
greater rate of
high frequency
attenuation causes
the
electromagnetic
field intensity of
the higher
frequencies to
appear stronger at
the perimeter than
the lower
frequencies, which
have a seemingly
more uniform
distribution. This
is why many
erroneously claim
that the higher
frequencies travel
in the conductor's
outer 'skin.' What
very few people
understand, and
this is the most
important aspect
of the wave
penetration, is
that the speed of
propagation in the
conductor itself
is incredibly
slow. Instead of
some high
percentage of the
speed of light,
the wave, in
copper for
example, travels
radially at
approximately 3
meters/sec at 50hz
and 60 meters/sec
at 20kHz. Compared
to the waveform in
the dielectric,
this is a low
level, grossly
time smeared
signal, and it
wreaks sonic
havoc.
"Note:
this wave-guide or
transmission-line
model of
electrical energy
flow is an
established
engineering/physics
principle that has
been used for
decades,
particularly in
high energy/high
frequency
applications
where, as in audio
applications,
these effects are
non-trivial and
must be accounted
for. In the mid
1980's, the
well-known and
respected audio
engineering guru
Dr. Malcolm
Hawksford of the
University of
Essex in England
was the first whom
I know of to apply
these concepts to
the audiophile
hobby in an
attempt to explain
why there are
sonic differences
among varying
cables designs.
His collection of
works, titled the
Essex Echo, remain
the most important
papers ever
published on the
subject, and
condensed/layman's
versions have been
published in some
audiophile
magazines. The
basic equations
behind all this
can also be found
in college texts
on engineering
electromagnetics
and
transmission-line/electromagnetic
wave propagation.
"There
are only two ways
to alleviate this
energy loss,
prevent time
smearing, and
create a conductor
that acts in a
more linear
manner. The first,
the method
employed in my
Silver cables, is
to utilize a very
thin ribbon. A
very small round
conductor would
also act linearly,
but cannot pass
much current.
Using multiple,
individually
insulated
conductors
increases current
carrying
capability but
also adds solid
dielectric and
mutual inductance
(strand
interaction)
degradations that
increase with the
number strands.
The only way to
avoid mutual
inductance and its
associated signal
smearing is to use
a single,
solid-core
conductor per
polarity. Special
weaves or
geometries (Litz
or any other) will
not eliminate this
basic electrical
phenomenon.
"The
Palladium cables
improve upon the
Silver by using
even thinner
ribbons. They also
employ a conductor
material with
superior
skin-effect
related
characteristics,
an advanced
palladium-based
alloy whose
properties
represent an up to
25-fold
improvement over
gold, silver,
copper, and
aluminum.
"I'll
stop rambling now.
Hopefully I've
explained why I
have gone to such
lengths to avoid
thick metal
anywhere in the
signal path and
use only single
conductors in an
air
dielectric."

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