Forum,

I have made some measurements and gotten results which are at odds with my
intuition.  I am wondering if someone out there can shed some light on this
subject.

I was interested in the losses associated with rf traveling on a twisted
shielded pair cable.  The scenario is that a length of this TSP cable is
exposed to an rf environment (as in a test chamber during IEC 1000-4-3
testing) and then the cable penetrates a bulkhead using a grounded connector
that provides excellent shield termination, and the cable continues on the
other side in the pristine rf environment of a shielded control chamber, say
for several meters.  The question is, how much rf signal is at the final
destination point vs. at the bulkhead.  The concern is common mode, not
differential mode.  Meaning that the twisted pair can be looked at like
coax, with an identical signal on both inner conductors relative to the
shield.  I expected losses that would be on the same order or lower than
that associated with off-the-shelf coax types like RG-58.  Instead my losses
were dramatically higher.

Following is my measurement technique.

I measured the transmission line impedance of the TSP in the following way.
I tied the center conductors together.  I shorted the center conductors to
the shield at one end, and measured the inductance, using an LCR meter.  I
opened the connection and measured the open circuit capacitance.  The square
root of the l/c ratio is the characteristic impedance.  I built matching
networks to get from 50 Ohms to the measured impedances which ranged from 15
- 25 Ohms for a variety of different cables.  For each cable, I built two
pairs of identical matching networks:

4 each: 50 to RC adapters

I used an HP 4195A network analyzer, over a range of frequencies 0.1 - 500
MHz.  The set up was as follows.  There was 16 dB of pad coming out of the
source (including the 6 dB splitter).  There was 10 dB of pad at the
reference and test ports.  Results showed little evidence of vswr.

Coming out of the source, there is the 6 dB splitter.  Between one port of
the splitter and the reference port, I inserted one pair of the matching
networks:

Splitter output connects to  50 Ohm to RC adapter connects to RC to 50 Ohm
adapter connects to reference port.

I connected the exact same sequence between the other splitter output and
the test port.  The network analyzer displayed the dB ratio of the test port
signal relative to the reference signal.  This would be the difference in
loss between each pair of matching networks.  If I had built them perfectly,
the analyzer should have shown 0 dB difference.  Actual differences were
under 3 dB.

Then I inserted the cable-under-test between the RC connections on the two
matching networks in the test port side.

The loss associated with cable-under-test (CUT) is the difference between
the losses measured with the CUT in place and with the matching networks
directly connected.

The numbers I got were considerably higher than even a high loss coax such
as RG-174.  Because real coax uses a much thicker dielectric material than
just the insulation around a TSP center conductor, my "gut feel" is that
losses should be lower than for 50 Ohm coax.  I expect that materials picked
to be dielectrics for coax have low loss tangents relative to wire
insulation, but I don't have a feel for whether the difference in loss
tangents can make up for the extra thickness of the dielectric in real coax.
Can any one tell me if either my test set up or my expectations are wrong,
and why?

Thank you.

Ken Javor

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