> 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/1asxej
http://cid-f9db37b8211ce831.office.live.com/self.aspx/Snippets/Multiplier%5E_basics.gif

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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