I needed a small capacitance (50-100nF, not discharged aggressively) periodically charged to 1200V as part of a project so I put together a little flyback converter with an off-the-shelf surface mount flyback transformer which works nicely.
Chatting later, a physicist friend asked why I couldn't just use a voltage multiplier. Turns out he didn't mean a few stages on the end of a flyback/boost/resonant driver, but literally chopping the 12V rail into an epic 100x charge pump!
I tried to use spice with vaguely realistic models of diodes, capacitor losses and parasitics to show why such long ladders don't work out in practice, but it stubbornly insisted on performing well in simulation.
Real-world demonstrations are more fun anyway, so I dropped 120x cheap B1040X 40V Schottky diodes (2 pence each on LCSC) and 120x 10u 35V 0603 MLCCs (2 pence each on LCSC; <1uF with DC bias of course, but that's fine) on a 30mm x 45mm board, probably stretching the creepage rules a little.
It stubbornly insists on working well in reality too. Driven at 500kHz from 12V with a little bootstrapped 4 x NMOS full-bridge from my spares pile, it charges fully in under 20ms. Stopping it at 1200V and discharging to 1000V through a 100k test load shows an effective capacitance of around 40nF, rising as it discharges further.
That's about right for the theoretical 4C/n with C roughly 1u - as predicted by Simsurfing with the 20V DC bias on these little capacitors, which I know are pushing the limits of class II dielectrics.
I'm very surprised that such a long charge pump works well, let alone ends up small and cheap. I guess my prejudice here is outdated... or maybe it has always been wrong?
Are they ever used directly like this without an inductive boost stage, e.g. in lower power applications? Feels like they might be quite good on the EMI front?