Sometimes, a quick lookup for an unknown term happens to unfold a story more interesting than the main reading. Such was when I've looked up for the term 'Franklin oscillator'.
The Franklin Oscillator, by the patent from 1930, is this:
Source: Franklin oscillator patent - US2028596 - page 1An oscillator made out of two identical common-cathode inverter stages (can be made as well with common-emitter transistors), chained one after another as a non-inverting amplifier, and with a resonant parallel LC tank to ground, that is very loosely coupled between the output and the input of the amplifier.
The US2028596 patent for the Franklin oscillator also claims a specific mechanically thermocompensated mechanism and arrangement for a variable LC tank, as in the Fig.1 and Fig.2 drawings.
The legend says Franklin oscillators can make very stable VFOs.
Another example, with BJT:
Source: http://www.arthropodsystems.com/FranklinOscillator/FranklinOscillator.html
To stay brief:
- very stable as a VFO (when powered from a well stabilised voltage)
- well behaved and easy to build, the 2 inverting stages can be anything: tubes, BJTs, FETs, CMOS gates, etc.
- L desn't require taps
- the LC parallel tank has one side grounded (advantageous for shielding a variable C or L, or for adding a varicap diode to ground, in series with C, so to turn it into a VCO)
- the LC is very loosely coupled to the amplifier, so thermal and other variations in the the amplifier have little to no influence over the LC resonance
- being very loosely coupled, the quality factor of the LC tank remains unaltered
- typical coupling to the LC tank is made with very small capacitors, a few pF when the oscillator is made with tubes, a few tenth of pF when with BJT (i.e. a 2pF for tubes can be made by twisting isolated wires - sometimes called a gimmick capacitor - depending on the number of twists it can give 1pF/inch, or 0.4 pF/cm - the capacitance can be reduced in circuit, by clipping away the length of the twisted wires)
- voltage feedback, if the negative impedance of the amplifier is >= R_losses of the LC tank then the circuit will oscillate, or apply
Barkhausen criterion to determine the oscillation condition
- the point with maximum amplitude oscillations and lowest distortions/harmonics is at the LC tank (the output signal can be taken from the LC, if a loosely coupled buffer with a high enough input impedance is added to the schematic)
Franklin oscillator seems to be one of the most obvious types of oscillators: a non-inverting amplifier with a resonant LC to ground in its positive reaction. I wonder why other types of oscillators (e.g. Collpits or Hartley) are taught in every RF101, while the Franklin Oscillator is never mentioned.
It's tempting to give it a try, and see how it behaves. Don't need any oscillator right now, but it has a certain elegance and simplicity, not sure why this oscillator seems so appealing.
There are plenty of schematic examples online, though I'm still not sure what are the must have of a Franklin oscillator. A positive feedback network, with a loosely coupled parallel LC to ground seems to be a must have, but does the amplifier has to have two inverting stages?
Would it still be a Franklin oscillator if some other non-inverting amplifier is used instead?