I think this idea is great mainly from an educational perspective - it clearly demonstrates the dramatic things that can happen through capacitive coupling, whether intentional or not.
I dont tend to use RF connectors (50-239 or the like) - my antennas on recent prototypes have used standard 6.35mm stereo jack sockets / plugs - particularly useful for directional antennas as they allow the antenna to be easily rotated.
The issue of antenna capacitance is an interesting one - its something I am playing with and recently changed my perspective on..
Large antenna capacitance is a real bother when one uses a series tuned scheme for linearization - and probably also if one uses a "tankless" series scheme - but its no bother for a directly connected parallel tank - with these one has a camparatively large tank capacitance anyway (usually 100pF or greater) and the antenna capacitance is simply in parallel with this - so even if the antenna components add up to 50pF, one can simply reduce the fixed tank capacitance if needed - A 455kHz IFT has 680uH || 180pF (454.9kHz) so a 1pF change (+1pF) gives 453.7 kHz, 1.2kHz/pF.. But its easy to increase the sensitivity, simply by adding a series inductor to the 680uH IFT - for example, a 5mH in series gives an adjustable 5680uH inductor, strap a 50pF across this (combined tank and antenna capacitance) and one gets an operating frequency 'round 295kHz, and a sensitivity of about 3kHz/pf.
The above gives no linearization - and its unusable in its raw form - but add electronic controlled capacitance, and one can 'squash' this excessive sensitivity and use it to implement linearization.
IMO, the 'bulk' antenna capacitance is only a bother with conventional theremin topologies - One gets into the habit of doing everything one can to minimise this, and avoids using screened cables etc because one usually gets into theremins via the conventional route - But I am starting to think that its a non-issue if your topology implements pure capacitive sensing, and isnt trying to be a musically linear sensor.. If the focus is on getting capacitive data which one processes and corrects further down line.
Fred.
Actually, some of what I said above is nonsense - The above facts apply equally to series and parallel tanks - they only dont apply when one uses seperate oscillator tank and antenna resonators and capacitively loads the antenna after the EQ inductor.. IMO, its this combination (Seperate tank and antenna resonant circuits) - which was invented for good reasons (linearity and antenna amplitude) which is IMO limiting for new designs.
I am really annoyed with myself for not seeing the issues above far sooner - My Skywave H1's were needlessly awkward to construct simply because I wanted the board close to the antenna, so ended up having to pipe power supply and audio wiring from the lower active loudspeaker (which contained the power supply and amplifier) up to the top speaker (which contained the theremin circuitry)
I could easily have had the theremin in the lower speaker with the other electronics, and simply run an RF shielded cable up to the antenna with its EQ inductor placed there - even if this cable had 40pF I could simply have reduced the tank capacitor by this amount.