I have an assignment for my Electronic Measurements and Instrumentation course, specifically me and my group were asked to perform time and voltage measurements using reflectometry on coaxial cables. We used an Agilent 33120A waveform generator and a HP 54600B oscilloscope.

One specific task was to measure the propagation delay over an adapted 5m coaxial cable: having plugged T connectors to both the scope's channels, we connected the waveform generator to the first channel, plugged a 5 m coaxial cable to both T connectors, and we adapted the line connecting a 50 ohm plug to the second T connector. This way, we could see approximately the same signal at the start and at the end of the cable, and measure the delay between the two signals. We executed this task using both a 1kHz square wave and the sync signal from the waveform generator, which apparently is a TTL output. From the manual: "For sine, square, triangle, and ramp waveforms, the sync signal is a TTL “high” when the waveform’s output is positive, relative to zero volts (or the dc offset value). The signal is a TTL “low” when the output is negative, relative to zero volts (or the dc offset value)".

Here is a comparison between the generated square wave and the sync signal:

(Comparison between the generated square wave and the sync signal.)

Here is a capture showing a generated square wave at 15MHz (upper limit of the waveform generator), and the related sync signal. Keeping in mind that the scope's f3 is at 100MHz (we will never see a real 15MHz square wave on this scope), you can clearly see that the sync signal and the "normal" output are generated differently.

15MHz square wave + sync signal

I'm not familiar with TTL modules (I know they are a BJT technology used in the manufacture of logic gates, but that's it), a bit of searching revealed to me that TTL signals are very badly suited to transmission lines because of their varying output impedance on their "high" and "low" levels. In fact, the displayed sync wave (connecting the sync output directly to one of the channels of the scope, reading voltage over an open circuit basically) is an approx. 4V square wave with a 400mV overshoot (approximately 100us long), and with an approx. 200mV DC offset, which is consistent with my findings (TTL low levels are 0-0,4V, while TTL high levels are 2,2V-VCC). If I read the voltage differential on the coax with the 50 ohm terminator plugged in, the overshoot completely disappears (and of course voltage approximately halves). Why is this? Is this related to that variable output impedance?

Another question is: time measurements are best taken using the ordinary square wave or the sync wave? The sync wave has a much faster rise time, so I'd point to the latter.

  • \$\begingroup\$ Try this: electronics.stackexchange.com/questions/90366/… - transmission lines need to be terminated for that reason. \$\endgroup\$
    – Andy aka
    Commented Dec 6, 2014 at 19:34
  • \$\begingroup\$ I know this. I'm actually enquiring over the nature of the signal, and its characteristics. The assignment's question is: "why does the sync signal have faster rise times? Is it best to use this signal or the generated 1kHz square wave to evaluate propagation delays over the cable?". I have added two pictures showing the difference between the generated signal and the sync signal, and an excerpt from the manual. \$\endgroup\$ Commented Dec 6, 2014 at 20:53

2 Answers 2


Well your pulse starts on your 50 transmission line, flies down to the end of the cable, and slams into your high impedance scope input. I just looked and your scope has a 1Meg Ohm input impedance. The wave then reflects off of that impedance and begins traveling back towards your source. When you apply the 50 Ohm terminator you have now matched the impedance of your transmission line with your cable and there is no reflection, but you will only get half of the voltage.

Take a look at this article by Johnson where he shows the reflection coefficient formula as:


You can see if your load impedance and transmission line impedance match there will be no reflection.

Also I think this series of three articles does a great job of explaining the details of all this.

  • \$\begingroup\$ This is clear to me, probably I didn't make myself understood. I have added information on the sync signal and a capture from the scope, comparing the generated square wave to the sync signal (both sent directly into the oscilloscope over a coaxial cable) in the OP. \$\endgroup\$ Commented Dec 6, 2014 at 20:29

The reason that the voltage of the sync signal halves when you terminate the cable is because the sync signal comes from a generator with a 50 ohm source impedance and the terminator is, ostensibly, 50 ohms as well.

Considering the transmission line between them lossless, that forms a 2:1 voltage divider, with the voltage across the load being 1/2 of the generator's open-circuit voltage.

If your sync signal has crispy edges, then it's a no-brainer; use it as the test signal and measure the delay of an edge from channel A to channel B.

With the 5 meters of coax between them and terminated at channel B, you should see something like a 20-25 nanosecond delay from channel A to channel B if your coax has a solid polyethylene dielectric.

  • \$\begingroup\$ I was thinking about this I feel like I'd rather use a sine wave to measure delay. If I use a square wave the rise time will degrade as the higher frequency components are attenuated, so some of my delay will be because of that. Maybe I'm over thinking it at these speeds/distances :) \$\endgroup\$ Commented Dec 6, 2014 at 23:16

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