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Coax
loss due to dielectric conduction
Updated February
23, 2007
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New page for March 2007!
Loss due to conduction in coax is the only loss mechanism that acts
independent of frequency, and independent of geometry! The
second point is not intuitive, but here we'll show you why it's
true.
In most cases, the conductivity
of a dielectric is so low that this term can almost universally
be ignored. PTFE is often used as a dielectric
in cables, its resistivity is around 1018 ohm centimeters!
(We don't have to tell you that resistivity is the reciprocal of
conductivity, do we? Engineers can never seem to make up their
minds which one to use...) But with the advent of micromachined
structures on semiconductor substrates like bulk silicon, you never
know when knowledge of this calculation might come in handy.
Did we mention that extremely
expensive EDA software such as Agilent's ADS doesn't feature the
contribution of dielectric conductivity in their coax models? We
can't explain why that is, but our coax download does it all, check
it out!
The first thing to do is to calculate
the the conduction per unit length, G'. Here, sigma is the bulk
conductivity of the dielectric. The calculation for G' is nearly
identical to the calculation for C', the capacitance per unit length,
in both cases you are integrating the bulk property from one annular
surface to another which results in a ln(D/d) term.

The attenuation constant due
to conduction is then:

A interesting thing happens when
you plug in the formula for coax characteristic impedance to the
above equation. The most exact equation for coax Z0 is:

Plugging the previous two equations
together we get:

Notice that G
is proportional to ln(D/d), while Z0 is inversely proportional
to it. So as G' increases, Z0 decreases (and vice versa).
Canceling the ln(D/d) terms,
simplifying the equation, and noting that R
is close enough to one for any material that you'd ever consider
for a dielectric so you can ignore it, you are left with:

Thus G
is not a function of coax geometry, it is only a function of two
bulk material properties of the dielectric, its conductivity and
dielectric constant.
As a final note on this topic,
if you calculate the loss of PTFE due to dielectric conduction,
you'll soon see that a PTFE coax cable from here to Mars has less
than a dB of conduction loss (approximately 10-13 dB/m)!
On the other have a coax connection using low resistivity silicon
will have loss greater than one dB per millimeter length!
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