GARTHWILSON wrote:
To see a square wave output of your 40MHz oscillator, you'll need an oscilloscope capable of at least about 400MHz and preferably more,
I patently disagree with this. The sum of a fundamental plus its 1st odd harmonic is plenty sufficient to see a square wave (though it'll exhibit lots of ringing on the display that doesn't actually exist in reality). Thus, to see a 40MHz square wave, a 120MHz scope is plenty.
Quote:
Additionally, the oscillator, especially at those frequencies, will not do nearly as well as it could if it's not in a board with power and ground planes or the traces are long and not terminated in their characteristic impedance.
The characteristic impedance thing is probably the culprit here. I know for a fact (and from first-hand experience) that a cable that is improperly terminated will exhibit higher losses per length than a properly terminated cable of the same impedance. Losses are also dependent on frequency: the higher the frequency, the greater the loss. Consequently, if an impedance mismatch occurs on the board with the oscillator, it's quite possible that all those odd harmonics are being strongly attenuated by the losses in the trace (e.g., they're being radiated as RF or are being shunted to ground through capacitive coupling some how). Thus, only the fundamental remains the strongest, and therefore, looks like a sine wave on the oscilloscope.
Just a hunch, of course, based on my experience. I know this because as soon as I replaced my RG-58U coaxial cable (3dB/10ft loss at 30MHz under properly loaded conditions) with 300-ohm twin-lead cable (0.3dB/10ft loss under the same conditions), I suddenly found that not only could I hear more remote stations better, I could rather regularly make contact with Australia on the 10m band with only 10W ERP. Before the change over, people only city blocks away couldn't hear my signal. Go figure.