I thought about adding a Pot but wasn't sure the value I would need
and how to hook it in correctly.

On Oct 11, 3:11 pm, GreyFox <[email protected]> wrote:
> I was measuring from the ground off the fuse to the anode pin with no
> tube connected. I did try the tube and I had nothing going on with the
> tube. Thinking it was DOA. Not sure thought I may have done something
> incorrect. I measured with the 180K resistor and a 270K resistor.
>
> John
>
> On Oct 11, 1:46 pm, Dekatron42 <[email protected]> wrote:
>
> > In most circuits with the EZ10A, and also the EZ10B, the current
> > through the tube should not exceed 1.3mA when the tube is used
> > together with cathode resistors of 6.8KOhm resistance (or 10KOhm if
> > they are capacitively decoupled with 560pF for higher counting
> > speeds).
>
> > With a supply voltage of 470V this results in an anode resistor of
> > 150KOhm and with an anode voltage of 560V the anode resistor should be
> > 220KOhm for the EZ10A.
>
> > The EZ10B can usually be used with the same anode and cathode
> > resistors but you might benefit from dividing the anode resistor into
> > two parts, one potentiometer in series with a resistor (the resistor
> > and potentiometer should have roughly the same value) the resistor
> > should be decoupled to ground by 22nF for counting stability.
>
> > These values results in a voltage drop of roughly 265 Volts in the
> > tube and it will result in a voltage drop across the 6.8KOhm resistor
> > of roughly 9 Volts, which is in accordance to the design parameters
> > for these tubes.
>
> > To drive the tube at low counting speeds you need a negative guide
> > pulse of roughly 50V and at high speed counting you need roughly 150V
> > negative guide pulses.
>
> > If you use the tube outside of these parameters, especially at higher
> > current it will degrade quite fast according to the articles I have
> > read, which is the main reason for some tubes not to work that are
> > sold on eBay.
>
> > On 11 Okt, 20:58, threeneurons <[email protected]> wrote:
>
> > > > Not sure what is going on but I checked the circuit and I am getting
> > > > 613VDC with the 180K Resistor (R3) in the schematic. I increased the
> > > > resistance to 270K and I still get 613VDC. Not sure why this is.
> > > > Anyone have a thought on why I'm getting 613VDC?
>
> > > > John
>
> > > On what side, do you get the 613V. If its the side away from the
> > > anode, then it may be okay. And it won't change with resistor. What's
> > > the voltage across the  dekatron (anode pin to cathode pin - any
> > > cathode) ? What's the voltage across the anode resistor ? Divide that
> > > number by your resistor value (used) to get the current.
>
> > > Dieter got a little carried away with the multiplier ladder. If you
> > > use capacitors that are too small, the ripple will be outrageous, so
> > > the average voltage won't go up to the calculated value. In the '120
> > > World' you really don't need more than 1.5x multiplication. REMEMBER
> > > 120V is the RMS (Root Mean Squared - or DC equivalent work) value. The
> > > sine wave really has a 165V peak value, and ~330Vpp (peak-to-peak)
> > > value. Look at the following drawing:
>
> > >http://snipurl.com/1asxejhttp://cid-f9db37b8211ce831.office.live.com/......
>
> > > Refer to image 'D'.
>
> > > If you put 120V (110V, 115V, 117VAC) RMS into that circuit, you'll get
> > > ~500VDC out, unloaded. The light load most dekatrons put on this
> > > circuit (assuming an appropriate anode resistor), should not induce
> > > too much ripple, so the voltage measured won't sage too much. On
> > > circuit 'D', the lowest located rectifier, and capacitor form a simple
> > > half wave rectifier & filter, which will output +165VDC, unloaded. The
> > > left most capacitor's bottom end is riding on the input AC signal.
> > > It's top end is tied to the anode of the rectifier, that's tapped off
> > > the +165V. Since this voltage is dynamic (moving), the top end will
> > > also try to stay in step with the bottom end (this is what the
> > > coupling caps in your stereo does). But its attached to the +165V
> > > (thru a rectifier). The bottom of the cap will make a 330V swing from
> > > -165V to +165V. When the swing is all the way down at -165V, the top
> > > is forced to +165V by current flowing thru the rectifier. This will
> > > charge that cap to 330V from top to bottom. As the sine wave goes back
> > > up, the top will still stay in step, which will make go over the 165V,
> > > so that diagonal rectifer (now being reversed biased) is switched OFF.
> > > When the input sinewave hits +165V, the top of the cap will be at
> > > nearly 500V (495 or there abouts). In the meantime, it would be
> > > charging the upper right cap. With no load, this circuit will present
> > > a DC voltage of close to 500V.
>
> > > In the 220V (220, 230, 240) world, you can get away with circuit 'C',
> > > which will give you 660VDC unloaded. Don't worry too much about the
> > > voltage.
>
> > > Dekatrons, like nixies (and LEDs) are current devices. Its the current
> > > flowing thru them that's important. And that's controlled by the anode
> > > resistor. You can use a 'test' resistor for temporary measurements.
> > > You need to measure (1) the actual supply voltage, and (2) the 'tube
> > > drop' voltage from anode to a cathode. Once you have those two, then
> > > you can determine the 'final' anode resistor value you want, from the
> > > specs given for that tube. (ie the anode or cathode current). The
> > > resistor will simply be supply voltage minus tube drop to give you the
> > > anode resistor voltage. Divide that voltage (anode voltage) by the
> > > desired current, to get the actual value, or close to it. Pick a real
> > > value made that's less than 40% away from that calculated ideal.
>
> > > In the Philips datasheet for the Z504S dekatron, the maximum allowed
> > > supply voltage is 1000V. That's why you see values from 400V to over
> > > 600V commonly used. It really ain't that critical, as long as you
> > > adjust your anode resistor, accordingly.

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