Ron Thompson wrote: > ... > receiving antenna is moved out of dead centre between the two radiating > plates (where the two fields from the two radiators should produce a > null point) it will capacitively couple to the closest plate and have a > voltage on it that is in phase with the closest plate... This approach sounds fine. One variation that might be interesting is to mount the radiating panel on the boom, but make that panel out of double sided PC board. Drive it with a center-tapped RF transformer. That way your 180 degree phase is on opposite sides of that panel and you can resonate the capacitance of the panel easily, which makes driving it easy. Now the pick-up plates will be stationary and close to the detector circuit and easily shielded with short lead lengths and you can null their output with simple summing which is then fed to a synchronous detector (an RF mixer) in order to recover the direction of displacement. Since the voltage on the radiating plate can be in the volts range and mixers can have microvolt noise levels, the potential exists for 120 dB dynamic range - now you've met many of your requirements. Everything mentioned above can be fairly hi-Q - read low loss - so power consumption can be restrained and the additional side benefit is hi-Q also results in good S/N levels which is necessary for low noise floors. I have to make additional comments on the area of VCOs. First, in response to my comment about noise in the power to your VCOs you mentioned using a 78L08 regulator. Unit IC regulators have many microvolt noise figures. It can be a substantial problem in low-noise instrument designs that require low noise power such as for references. The problem stems from the use of buried zeners or the even noisier band-gap references internally. The standard solution is to use lots of RC filtering but this becomes difficult at really low frequency - frequencies such as in seismic records. One solution was to go to mercury batteries as a reference - very low noise figures. Second, for low-noise in a VCO, it is typically locked to a low-noise crystal oscillator, which effectively gives it hi-Q. Your application by definition has to be un-locked. This is a recipe for noise -- lots of it. Hi-Q LC oscillators are possible, but the detector scheme would have to change. An example I can think of is to use a high frequency in the variable LC oscillator (not a VCO). Implement the oscillator with the boom causing variable capacitance, which can be done without requiring any wires, so only a plate or tube is on the end of the boom. Take the oscillator output and use a D-flop mixer using a crystal as a reference to bring the frequency down to the audio range. Now you can go a couple of ways. A CMOS VCO such as a 4046 locked to the audio note with the control voltage used as the output measure of displacement. Or feed the the audio frequency into a freq-to-voltage IC. (National used to have one and I believe there are others.) This can be a low current scheme and low noise that has no sensitivity to power line frequencies. Regards, Charles R. Patton __________________________________________________________ Public Seismic Network Mailing List (PSN-L)
Larry Cochrane <cochrane@..............>