[Lowfer] Lowfer KE
jrusgrove at comcast.net
jrusgrove at comcast.net
Sun Nov 22 07:12:44 EST 2020
Kasey
Can drop a couple 27 pF silver mica caps in the mail ... along with the resistors. Just say the word.
Jay W1VD
----- Original Message -----
From: J D <listread at lwca.org>
Reply-To: Discussion of the Lowfer (US, European, & UK) and MedFer bands <lowfer at mailman.qth.net>
To: <lowfer at mailman.qth.net>
Sent: 11/22/2020 2:26:24 AM
Subject: Re: [Lowfer] Lowfer KE
________________________________________________________________________________
Kasey, it would appear from your schematic that a few components may be
missing, thereby preventing your oscillator from being as stable as it
needs to be. This same situation is found in a commercially made
sorta-kit rig for 22 meters, and beacons using it there can often be
identified by their tendency to wander or even outright jump around in
frequency from day to day.
A Pierce oscillator needs capacitance from both legs of the crystal to
ground as part of a phase shift network. There is stray capacitance
present, of course, without which it would not oscillate at all; but
that is neither of sufficient magnitude nor stability to ensure reliable
oscillation at the design frequency of the crystal. A good starting
value for capacitors for a typical 3 MHz parallel resonant crystal would
be 27 pF each.
In addition, there needs to be a series resistor between pin 10 and the
crystal. It serves three functions that each affect frequency stability
to a certain extent: it isolates the crystal somewhat from the complex
impedance of the gate output, it limits current and thereby power
dissipation in the crystal, and it is part of the phase delay network.
As a rough first approximation, I'd suggest 1 K, maybe as high as 2.2 K.
Finally, the shunt resistance across the crystal could be a little
higher in value for 3 MHz operation, such as 3.3 M to 4.7 M. It's not
terribly critical, but it is preferable to operate it with as high a
value as will allow for reliable startup. Lowering the operating Q of
the crystal with a low parallel resistance could allow a crystal to jump
too easily between primary resonance and any secondary resonance modes
it may have.
These comments are some basic rule of thumb guidance. For more detailed
treatment of Pierce oscillators implemented with logic gates, I believe
Crystek still offers this article:
https://www.crystek.com/documents/appnotes/pierce-gateintroduction.pdf
John Davis
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