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Slotted
line measurements
Updated March 30,
2009
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Note to readers... this discussion
of slotted line measurements is here mostly for historic value.
It will help you understand why microwave engineers use voltage
standing wave ratio (VSWR) as a requirement, even though a "more
modern" way to measure impedance mismatches is to measure S-parameters
using a network analyzer.
New for April 2009! Thanks
to Chuck we now know how to measure load impedance
using the slotted line!
Not that long ago, in a time
before network analyzers, engineers of yore used something called
a slotted line to measure voltage standing wave ratio. You might
turn up such an instrument if you work in a lab that is more than
25 years old. Basically it is a coax line with a slot down one side
where a probe can be moved longitudinally to measure varying electric
field strength. The probe has a detector that converts RF energy
to DC voltage, so you can measure peaks and valleys using an voltmeter.
For circuits that were extremely mismatched (or open or short circuited),
the peaks and valleys are the most noticeable. The ratio of the
peak voltage to the valley voltage was the most directly calculated
piece of data you can get with a slotted line... hence "voltage
standing wave ratio".
Using a slotted line, you could
also measure an unknown frequency by measuring the distance between
the voltage peaks and noting that the distance is 1/2 wavelength.
Here's some slotted line equipment
that we found recently on Ebay (none of which sold!)
Hewlett Packard
C17540 HP 816A

Alford 3300

C17452 General
Radio 900-LB

Let's look at a slotted line
measurement. Suppose you recorded the detected voltage along a 25
centimeter slotted line. The data might look like this:

In this case, the peak voltages
are about 1.3 volts and the nulls are about 0.7 volts. That's a
standing wave ratio of 1.85:1.
What else can you tell from this
measurement? You can measure the frequency of the source (if it
was unknown), if you know the dielectric constant of the slotted
line (1 if it is air dielectric). The distance between nulls is
a half wavelength. You should always measure between the nulls,
not the peaks, because they are much sharper and easier to discriminate
in distance (in spite of the above graph where they look the same!)
From the plot, if the X-axis is in centimeters, we could estimate
a wavelength of 6.25 cm (four wavelengths in 25 centimeters). Just
divide that into the speed of light (30,000,000,000 cm/s) and you
will get an answer of 4.8 GHz. Thanks for the correction, Renato!
If anyone has further interest
in the topic of microwave measurements as they were done in the
1960s, we recommend this book : "MICROWAVE
THEORY AND APPLICATIONS" by Stephen F. Adam of Hewlett Packard,
you can probably find a used copy somewhere. Or just borrow a copy
from an old dude out in your lab!
How
to measure characteristic impedance
This info came from Chuck...
thanks!
You can measure impedance
of the load with the slotted line. After you measure the VSWR
and draw the VSWR circle on the smith chart, you can mechanically
measure the distance from the unit under test to the probe (parked
at a peak or null) Then replace the load with a short or open
and measure how far you have to move the probe to the new peak
or null. Convert the length to wavelengths and rotate the appropriate
way around the smith chart. Good stuff (I didn't think so as a
student, but I do now).
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