I forgot that I had a 50 ohm load on the scope end of my cable for that picture. The audio output is cap coupled. That's why the short pulse with long exponential tail. If I use 1M input at the scope it is a square pulse >200 uS but still has that glitch on the leading edge.

I put a simple RC filter on the output; the rise time gets stretched but the negative glitch becomes a step. Good enough for the counting.


On 6/5/2011 3:53 AM, Bruce Griffiths wrote:
Maybe, but the circuit diagram indicates that the pulse that you see is nothing like what it should be.
There may well be a circuit fault.
The circuit already includes a monostable.

Bruce

Rex wrote:
We are getting pretty far afield of my original counter triggering question.

As far as I know, any specific quenching is only necessary for achieving the highest counting rates which isn't involved in my measurements, so far as I know.

Like I said, this is a 1960's CD counter. Pretty impressive that it still works. They did a pretty nice job with minimal components, I think. If you really want to see the trivial details, here is the circuit (updated by someone to make it more logical from it's original drafted version).
http://www.cs.utah.edu/~hatch/images/lionel.gif

I am counting out of the suboptimal Audio output.

I did change the original "hotdog" tube to a pancake style detector for these measurements.


On 6/5/2011 2:12 AM, Bruce Griffiths wrote:
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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