[time-nuts] Fluke PM6681 triggering
Bruce Griffiths
bruce.griffiths at xtra.co.nz
Sun Jun 5 09:12:52 UTC 2011
Is the GM tube internally or externally quenched?
Its necessary to quench each avalanche discharge either by using an
internal quenching gas (eg a halogen) or to use suitable circuitry to
ensure the discharge terminates.
Bruce
Rex wrote:
> Bill and Bruce,
>
> Clearly, fixing the messed up signal is the proper approach. What you
> are missing is that I got a shiney new (for me) expensive hammer and I
> thought that it should be able to drive defective nails. :)
>
> I got an off-list reply that suggested that hold-off affects the
> counter gating -- which either doesn't matter in this totaling app or
> complicates it. He also suggested using the negative slope of the
> pulse to trigger. Doh! The negative slope is more gradual and would
> affect timing accuracy, but that doesn't matter in my counting situation.
>
> Oh, and as reply to the question of more detail on where the signal
> comes from, this is a 1960's CD-700 (civil defense, yellow) gieger
> counter. The signal is the earphone output. In the future I think I'm
> going to make my own circuits to connect to a geiger tube or a
> scintillator/PMT MCA application, but that is even further from
> playing with the nice new counter.
>
> Thanks for the feedback -- any more welcomed.
> -Rex
>
>
> On 6/5/2011 12:42 AM, Bruce Griffiths wrote:
>> A Geiger Muller (GM) tube produces an output pulse as a result of an
>> avalanche discharge in the gas filled tube initiated by the passage
>> of ionising radiation through the tube.
>> A high voltage is initially maintained between an outer usually
>> cylindrical electrode and an inner small diameter wire electrode. The
>> discharge current develops a voltage across a resistor in series with
>> the inner electrode. The pulse amplitude is relatively large and
>> little gain is required to drive a speaker.
>>
>> Pulse shaping using a suitable differentiating and integrating RC
>> time constants is typically used to shape the pulses and maximise
>> the SNR of signals from scintillators and proportional counters.
>> For Geiger counters the signal is so large that such shaping to
>> maximise SNR isnt usually required.
>>
>> Using a non retriggerable monostable to define the deadtime in
>> nuclear counters is relatively common.
>> The pulse risetime for a GM tube is relatively slow so that something
>> like a 74HC series monostable should suffice.
>> An HCMOS monostable also has the advantage of a high input impedance
>> so that little or no amplification should be necessary,
>>
>>
>> Bruce
>>
>> WB6BNQ wrote:
>>> Hi again Rex,
>>>
>>> I should have asked these questions in the first place.
>>>
>>> How are you connecting the Fluke to the geiger counter ?
>>>
>>> Is this a signal that drives a speaker or some other kind of noise
>>> maker ?
>>>
>>> What happens if you load that line with some capacitance like 1 uf
>>> or more ?
>>>
>>> If the capacitance helps you will have to experiment with the value
>>> so as to not
>>> completely destroy the pulse shape. Never played with a geiger
>>> counter so have
>>> no real idea how they do the noise making.
>>>
>>> Bill....WB6BNQ
>>>
>>>
>>> Rex wrote:
>>>
>>>> I recently picked up a Fluke PM6681 counter (same as a Pendulum
>>>> CNT-81).
>>>> Looks like a sweet device.
>>>>
>>>> I was just trying to use it for a not-so-much-timing purpose and was
>>>> hoping to find an expert here who might help me with a triggering
>>>> question.
>>>>
>>>> I just set it up to count total pulses, over a 5 min interval, coming
>>>> randomly out of a geiger counter. Basically I set it up and it works
>>>> except for a subtlety. The pulses out of the geiger counter are not
>>>> clean. At a low count rate they have a big glitch on the leading edge.
>>>> Here is a picture of the pulse:
>>>> http://www.xertech.net/geiger/single.jpg
>>>>
>>>> The glitch causes the count to increment by two on each event except
>>>> that when the pulse rate gets high the pulse shape changes causing the
>>>> the glitch to smooth out and the peak amplitude to drop, like this:
>>>> http://www.xertech.net/geiger/multiple.jpg
>>>>
>>>> If I set the trigger voltage on the counter to just above the glitch
>>>> peak I can get proper counts, but finding a sweet spot on the changing
>>>> wave shape is not ideal.
>>>>
>>>> I thought I could use the counter's Hold Off feature to get a clean
>>>> solution but it isn't working as I expected. Reading the Operator's
>>>> Manual I thought that the Hold Off period started at a trigger
>>>> event and
>>>> would prevent another trigger event until after the hold-off period. I
>>>> thought I could set the trigger level to occur around the middle of
>>>> the
>>>> glitch rise (about 3 volts) and set the hold-off time for 1 uS or more
>>>> to prevent a 2nd trigger on the big rise just after the glitch. I
>>>> tried
>>>> hold-off values of 250 nS through 20 uS, but I still see the count
>>>> incrementing by two on the glitchy pulses.
>>>>
>>>> I'm wondering if anyone has experience with this counter and can
>>>> tell me
>>>> if I have mis-understood the Hold-Off function. Or maybe it has
>>>> something to do with me using Total A-B mode. The Op Manual covers
>>>> a lot
>>>> of ground, but it isn't the easiest to follow the finesse stuff unless
>>>> you happen to need to do exactly what they are showing in an example.
>
>
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