In the July/August 2008 QEX magazine there is an article by VE5FP
"Some Thoughts On Crystal Parameter Measurement" that may be of
interest.

On Sat, Jun 4, 2016 at 11:01 PM, Bob Camp <kb...@n1k.org> wrote:
> Hi
>
> There are two things you may be talking about:
>
> 1) The pressure springs on things like FT-243 holders, they are generic 
> springs.
>
> 2) The connection leads on plated blanks, they are indeed strange *and* 
> soldering to the blank is a big problem.
>
> I’m guessing you are in bucket number 2.
>
> Bob
>
>
>> On Jun 4, 2016, at 1:41 PM, Mike Cook <michael.c...@sfr.fr> wrote:
>>
>> Thanks all for your advice, hints, tips and links. Lots to read , do and 
>> some hardware to check.  I don’t have a frequency generator so I’ll have to 
>> go another route.
>>
>> Oh. One last Q. Has anyone tried repairing the « spring » wire electric 
>> connections on large quartz plates. In one large unit I have they had 
>> corroded and dropped the plate, luckily no damage.  I have done one, but I 
>> have no Idea what the original wire composition was so have certainly 
>> induced some stray capacitance/resistance. It is possible that it was a 
>> filter rather than a frequency source as it was not in a vacuum.
>>
>> Have a good one.
>>
>>> Le 4 juin 2016 à 18:49, Bernd Neubig <bneu...@t-online.de> a écrit :
>>>
>>>
>>> Tim Shoppa wrote:
>>>> The Pierce logic-gate-biased-active oscillator is pretty reliable to start 
>>>> and will oscillate somewhere with most crystals from kHz to MHz.
>>>> As you found out, it will often come up on one of many overtones.
>>>> To reduce chance of coming at an overtone, a series resistor from logic 
>>>> gate output to the crystal is often enough. If not, a RC low-pass will cut 
>>>> down even further (although of course adding phase shift.)
>>>
>>> This is certainly the easiest and fastest way for a go/no-go test and to 
>>> find the approximate resonance frequency.
>>> In the attached circuit diagram make CX1 and CX2 about 10 pF and RGK 
>>> several MegOhms.
>>> The inverter gate should be preferably an unbuffered HCMOS or other fast 
>>> inverter.
>>> For crystals in the MHz range you can replace RV by a short, for kHz 
>>> crystals make it a few kOhms. If testing small watch crystals @ 32768 kHz 
>>> or around, RV should be 100 kOhm at least. RV reduces the crystal drive 
>>> level (RF current) to an acceptable level to avoid overloading or even 
>>> damaging of the crystal. For low frequency crystals the RV-CX2 lowpass also 
>>> avoids start-up at the overtone.
>>> It is recommended to add a second inverter gate at the output to isolate 
>>> your oscilloscope or counter input from the oscillator stage. Add some >330 
>>> ohm in series to the output of the 2nd inverter, if you connect a coaxial 
>>> cable. Then terminate the coax at the oscilloscope or frequency counter end 
>>> with 50 Ohms, so the square wave form will be roughly maintained.
>>>
>>> In this circuit the crystal will not operate at its series resonance, but 
>>> at a load resonance with load capacitance of something between 8 pF and 10 
>>> pF (depending on the inverter input and output capacitance plus the stray 
>>> capacitances of your test fixture).
>>> If you want to operate the oscillator at a (low) overtone, such as 3rd (or 
>>> maybe 5th), you must add a series combination of 10 nF plus an inductor in 
>>> parallel to CX2. The 10 nF is to avoid DC short-circuiting of the output. 
>>> The inductor together with CX2 must have a resonance frequency mid between 
>>> fundamental mode and 3rd overtone (not at one of them). So the tuned 
>>> circuit acts like a capacitor at the 3rd OT and is inductive at fundamental 
>>> mode (thus the phase condition for oscillation is not fulfilled at the 
>>> fundamental mode)
>>> Have fun
>>>
>>> Bernd
>>> DK1AG
>>> <Pierce_Logic_Gate.gif>_______________________________________________
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>>
>> "The power of accurate observation is commonly called cynicism by those who 
>> have not got it. »
>> George Bernard Shaw
>>
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