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Dielectric Soakage Demo

@electrace/dielectric-soakage@1.0.0 · CC-BY-4.0
effect worst_in recovery 0.5–10 %
The actual schematic inside this block — every part is explained below.

Dielectric Soakage — the capacitor that recharges itself

Charge a big capacitor. Short it dead with a wire — voltmeter reads zero. Now take the wire off and wait. The voltage climbs back on its own, from nothing, with nothing connected. It looks like the capacitor is generating energy out of thin air.

It isn't. It's dielectric absorption — soakage — and it's one of the most uncanny things on an electronics bench.

What's really happening

A capacitor's dielectric isn't a single, perfect insulator. Under voltage, its molecules polarize — and some of them are slow. The bulk of the charge sits on the plates and responds instantly. But a fraction soaks into the dielectric, into dipole states that take seconds to minutes to line up and just as long to relax.

When you short the cap, you drain the fast charge on the plates in an instant — voltmeter reads zero. But the slow, soaked-in charge is still there. With the short removed, it leaks back out of the dielectric and onto the plates, and the voltage reappears. A big electrolytic can recover several percent of its original voltage this way.

Model it as a fast capacitance in parallel with a ladder of slow R-C states (dielectric relaxation). The recovered voltage is real stored energy that the quick discharge never reached — not a measurement glitch.

Why it matters

  • It can bite you. This is why big capacitors ship with a shorting strap, and why a "discharged" microwave-oven or power-supply bulk cap can recover to a dangerous voltage minutes after you thought it was safe. Short HV caps through a resistor and leave the strap on.
  • It corrupts precision analog. Sample-and-hold circuits and integrators avoid electrolytics and high-K ceramics (X5R/X7R) for exactly this reason: the soaked charge bleeds back and leaves a "memory" of the previous value on the held node. Film (polypropylene) and C0G/NP0 ceramics have almost none of it — which is why precision designs pay for them.

The effect is strongest in electrolytic, tantalum, and high-K ceramic caps; nearly absent in film and C0G. The bigger and more "electrolytic" the capacitor, the spookier the demo.

Watch it explained

Exposed nets

chargein · signal
measout · signal
gndin · gnd

Inside this block

R1
1k
charge/bleed resistor — limits inrush while charging C1 and gives a defined, gentle path; the soakage recovery happens AFTER this is disconnected, from inside the cap itself
C1
4700uF
the star: a big electrolytic. Its dielectric stores charge in slow dipole states a quick short can't empty — so it 'remembers' and recovers. The bigger and more electrolytic, the stronger the effect
SW1
short
the shorting strap. Press it to dump C1 to zero — but it only empties the fast bulk charge. Release it and the slow dielectric charge leaks back onto the plates: the voltage climbs from zero on its own

Limits & gotchas

physics.note 0A real dielectric isn't one capacitance — it's a fast bulk capacitance in parallel with slow, deep dipole states that charge and discharge over seconds to minutes (a Maxwell-Wagner / dielectric-relaxation network). A quick short empties the fast part; the slow part keeps its charge, then bleeds it back onto the plates. The recovered voltage is real stored energy, not a measurement error.
danger.note 0This is why big capacitors ship with a SHORTING STRAP and why a 'discharged' high-voltage cap can bite you minutes later — a microwave-oven or PSU bulk cap can recover to a dangerous voltage after you thought it was safe. Always short HV caps through a resistor and leave the strap on.
design.note 0Why sample-and-hold and integrator circuits avoid electrolytics and X7R: the soaked charge bleeds back and corrupts the held value (a 'memory' of the previous sample). Precision analog uses film or C0G for exactly this reason. Soakage also skews fast-settling references and slows true RESET of a charge node.
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