Bill,

I did a two sets of measurements using different methods. In the first, I 
watched the two waveforms in dual trace mode.  The Trimble was on channel 1 
(stationary) and the LPRO 
was on channel 2 (slowly drifting to the left).  I started timing when they 
were phase (Channel 1 and Channel 2 occupied the same trace), watched the LPRO 
waveform drift through 
180 degrees out of phase and then continue until the waveforms were back in 
phase, at which time, I stopped the clock.  

In XY mode, I started timing from a right slanting diagonal (in phase), watched 
the form become a circle (90 degrees), saw it collapse to a left slanting 
diagonal (180 degrees out of 
phase), expand to a circle (270 degrees out) again and finally back to a right 
slanting diagonal (in phase), at which point I stopped the clock.  The 
progression looked like this:
/O\O/ 

So, my answer to your question is yes and no.  Yes, I only counted the time 
until it returned to the same position.  No, I didn't ignore the 180 degree 
state.

Tom VB, Thanks for your calculation (100 / nS / 182 S = 5.5e-10): it feels more 
descriptive than the method I used.

Joe, in the first experiment above, I used your suggestion (triggering on 
channel 1 and watching channel 2 slide to the right.)  I have to think about 
what the drift direction means 
(your answer has an intuitive ring to it - moving right because the wavelength 
of the lower frequency is longer?)

Thanks all for all of the replies.

I'm afraid I've got the bug...  (I found myself looking at a cesium clock on 
the web this afternoon.)

Mark


Silly question but I thought I would ask just the same.

By in phase to in phase, and to make it clear, you did mean IF you selected the 
slant figure that went from bottom left to upper right, as the start point, 
that you only counted
the time until it returned to the same position ?  In otherwords you ignored 
the slant from upper left to lower right (the 180 degree position) while 
counting the rotation ?

Bill....WB6BNQ



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