I don't think that this describes the general usage of the terms. The said symmetrical circuit is usually designated "full wave" CW multiplier, it's quite common to name the present circuit CW multiplier as well.
Right, the nomenclature has become hard to nail down.
These articles agree with you. I have no basis to disagree.
http://en.wikipedia.org/wiki/Cockcroft–Walton_generator
However I have encountered several articles on the internet over the years. I see more than one name is connected to the multiplier in this thread. There is C-W and Villard and Greinacher.
For my own part, I find I need to give each of my circuit files a concise title which is informative.
So I've gotten in the habit of beginning with the simplest voltage doublers...
(a) one of which is based on the Villard cell (but which one source credits to Greinacher),
(b) the other based on a bridge of two half-wave supplies at opposite polarity (commonly credited to Greinacher but which one source calls the Delon doubler).
Then branching out to more complex multipliers, I add the half-wave parallel, full-wave parallel, series-parallel...
Then there is the type of supply, whether (a) AC sine waves, (b) pulsed DC alternating with high impedance, or (c) supply V alternating with zero ground... These all give different output levels.
So I have settled on a convention for giving names to my collection of voltage multipliers. The goal is to create names with quick recognizabilty, and which extend logically from the simple doublers as mentioned above. In regard to C-W multipliers, it is most frequently characterized as having several stages of Villard cells, mirrored above and below a zero ground. The developers for which it is named used it to boost a 200 kV supply to 800 kV. An article clarifies that it drew on the Greinacher design.
I have a hunch it will be impossible to create an orderly system of categories for all these varieties of voltage multipliers.
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Various web links in addition to those given above:
C-W history re early particle accelerators
shows a schematic not too different from the one in this thread
Wikipedia article
subheads include Villard, Greinacher, bridge, Dickson types
http://en.wikipedia.org/wiki/Villard_circuit#Villard_circuit
Jochen's high voltage page
mentions Greinacher, Villard, Villard cascade
http://www.kronjaeger.com/hv/hv/src/mul/
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However from the simulation I measure a ΔV = 140V & 2δV = 38V, but from the Kuffel equation with all the capacitors all equal to C I calculate a ΔV = 26.4V & 2δV = 7.2V which is quite the discrepency.
Why is this?
I don't know if current drain is factored into the equations, but a 10M load will allow the volt level to rise faster than a 1M load.
Even when the multiplier reaches an equilibrium (or maintenance) condition at over 5.9 kV, the 1M load draws bursts of a few hundred mA greater than the 10M load.
In case you would like to try measuring the results in a different simulation...
I am using Falstad's animated interactive simulator. It can export a link, below.
Click it and it will open the falstad.com/circuit website, load my schematic, and run it on your computer. (Click Alllow to load the Java applet.)
http://tinyurl.com/abm67qy
If you watch closely you will see the sequence in which the capacitors charge.
You can set the scope traces to show V or A, min and max readings, etc. Right-click on a trace and select what you want.
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