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![]() Thanks Craig for the clarification that the transmitter frequency for all transmissions to Pioneer 10 was the same and produced by a circuit that multiplied 96 in the early days;48, later, times a very precise 24 MHz local oscillator frequency And that this then could produce a very reliable difference in the received frequency and the transmitted frequency. My question: What is ratio of error sum of squares around the selected frequency to the sum of squares around the mean? Does item 101 Average Doppler Residual in the NASA data tape have something to do with the numerator of this ratio eg 3 times the sq rt of numerator would lead to a 99percent confidence interval for the true received doppler shift? Ralph Sansbury The process of digging the weak received signal out of noise as I understand it involved the representation of nanosecond voltage variations as a Fourier series with the largest weighted sine component of frequency around 2292MHz and the other sine components much smaller. The specific phase and frequency is detected using filters, Fast Fourier Transforms and Phase Locked Loops. And if you subtracted the received voltage values at each nanosecond or fraction of a nanosecond from those predicted by the detected frequency and phase, you would get a set of numbers that was normally distributed around zero indicating that these differences were noise. Of course if the component of frequency in the expected range has the same weight as those in other ranges then this would indicate that it too was noise also. If the sum of squares of the observed around a predicted set of values is as great as the sum of squares about the mean of the set of values then the predicted set of values is worthless and I suppose some sort of criteria is the basis for saying that the receptions from Pioneer 10 are now lost in noise. It would be nice to get a little more clarification on this point eg What is ratio of error sum of squares around the selected frequency to the sum of squares around the mean? Does item 101 Average Doppler Residual have something to do with the numerator of this ratio eg 3 times the sq rt of numerator would lead to a 99percent confidence interval for the true received doppler shift? Ralph Sansbury "Craig Markwardt" wrote in message news ![]() "ralph sansbury" writes: Hi Craig, Re the transmitter frequency subtracted from the received frequency to the get the doppler shift and motion of Pioneer 10 relative to the earth at any specific time. If the multiplier is exactly 48 for the DCOcase but 96 earlier and this corresponds to something specific in the phyical circuit, that would be ok. (What does it correspond to?) The hardware has a fixed integer multiplier between the reference oscillator and the transmitted frequency. For the VCO the multiplier was 96, for the DCO it was 48. This is not a tunable parameter, i.e. it is fixed exactly by the electronics and microwave components of the oscillator and amplifier. The "choice" of 48 vs. 96 comes in the modeling software. The multiplier in the software must match the multiplier used in the hardware. There is no subjective choice involved. Exactly and that is my question???? If the milliHz terms supposedly used to show a small anomalous acceleration would have been changed by using a different multiplier and there is no independent reason for choosing 48 or 48.1 etc, then there is a problem!!!! And, to reiterate, there is no fitting or tuning involved in the DCO multiplier. Another problem is how do we know the transmitter frequency was always exactly the same as the frequency produced by the DCO times 48? Because that is how the system was designed, tested and productively used for more than a decade. |
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