Somewhere in the near future, I’m hoping to experiment with building my first superheterodyne receiver. While I may be putting the cart before the horse in working on new receivers before putting up a proper antenna, until the weather kindly agrees to stay nice for more than one day at a time, it’s the soldering station for me.
An essential part of a superhet receiver, and the part I’m excited to experiment with, is the IF filter. The matching (or at least characterization) of the motional parameters of a few crystals is critical for filter design, so to that end, I put together a simple test oscillator a la G3UUR to try matching some crystals.
The G3UUR is a simple Colpitts oscillator with a buffer, which you are intended to attach to a frequency counter. A small bit of machine header allows for the insertion of individual crystals for testing. A SPST switch allows for one lead of the crystal under test to either be shorted to ground, or grounded through a small capacitor. By measuring how much the frequency of the crystal is pulled by added extra capacitance to the oscillator, we can calculate some basic parameters of the filter, namely the equivalent series capacitance and inductance.
Since I don’t have a nice diamond core drill bit as suggested by others, I made my own sloppy island pads using a engraving bit and my cheapo Harbor Freight knock-off Dremel. Though it’s not a particularly high powered tool, it eats through the copper on copper-clad with ease. Would definitely use this method again, it was tremendously easy. It also allows for the creation of oddly shaped islands, sad for making loops to attach power or ground leads to.
The G3UUR method is very simple: place the crystal in the oscillator with its lead grounded, and read off the frequency on a frequency counter. We’ll call this the base frequency, f. Then open the switch, so that the crystal is only grounded through the capacitor Cs, and read off the frequency again. (It’s worth measuring the capacitance here, rather than trusting the labelled capacitance.) The difference between the two frequencies we’ll call ΔF. The capacitance of the crystal itself (measured across the leads with a meter). we’ll call C0. The motional parameters of the crystal are then:
A quick experiment on a miscellaneous 9.838 mhz XTAL I had lying around gave results of 11 fF and 23.8mH, which are within the realm of possibility for a crystal of this size. More encouragingly, a June 2006 paper from Jack Smith K8ZOA suggests that the simple G3UUR method seems to give results within about 5% of more complicated and exact methods, like using a calibrated Vector Network Analyzer or performing phase comparisons of frequencies across the crystal.
Hopefully this is the first step toward building a “good enough” three or four crystal filter for a superhet receiver.
Hear you on the air!
73