On 4/3/14 11:17 PM, Chuck Forsberg WA7KGX wrote:
One needs to know the carrier frequency.  Must be a high quality reference
for the Cassini transmitter.

Two way measurements are most likely here (although Cassini does carry a USO). So the downlink is locked to the uplink which comes from a maser. The design of the transmit and receive system to hold that performance all the way through the chain is a challenge.

Interestingly, since the light time to Cassini is hours and hours, you need a *really* good clock on the ground, because you're comparing the phase of a signal you radiated several hours ago with the phase of the signal you are receiving now.


To put this in perspective.. at a range of a bit more than billion km (one way) the light time is a bit less than 5000 seconds,or 10,000 seconds round trip. So there are 4.2E13 cycles of the down link signal between Saturn and Earth. The Allan Deviation is on the order of 1E-15, so we are typically measuring the phase of that signal to a few degrees.

So, things like the physical temperature of the 70 meter DSN antenna make a difference. If the optical path is, say, 100 meters, and the temperature of the dish changes 1 degree C, what's the phase change? Well, steel has a CTE of about 13ppm/degree, and 13 ppm of 100 meters is about 1mm, which is about 10 degrees phase shift at 8.4 GHz (lambda = 36mm)

Solid Earth tides also feature into this.


I will point out that *measuring* the performance of the radio on the ground in the lab is quite a chore. You can easily see the air conditioner cycling on and off (that bump in Adev at 1000 seconds) and diurnal cycles in temperature. most of this affects things like the cables and connectors in the test setup.

And woe to the rookie engineer who thinks they can make the measurements with any old signal generator from loan pool.

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