Interactive Capacitor & RC Converter
Drag the charge on a live capacitor schematic, scrub the V(t) curve in real time, decode SMD code 104 to 100 nF, and read all 10 capacitance units from attofarad to statfarad - in audio, RF, power, supercap, CGS physics, or SMD context.
Quick Conversion
Formula: nF = µF × 1000
1. Pick your context
2. Audio circuit
Drag horizontally on the schematic to manually scrub the charge fraction. Yellow electrons flow while charging.
Drag along the curve to scrub time. The marker, schematic, and unit table all stay in sync.
3. All 10 units
Time constant & cutoff
SMD marking decoder
Where this converter shines
Audio crossover design
Pick the crossover frequency, watch f_c update with the chosen C and 8 Ω load. Bipolar coupling caps for tweeters, big film caps for woofers.
RF matching networks
L-section and Pi-network design in pF. NP0 / C0G ceramic presets with 50 Ω default resistance to keep impedance math intuitive.
SMPS / DC-DC sizing
Bulk and output caps in µF / mF, with low-ESR mΩ resistors. Ripple math gets the right intuition from the live charging curve.
Snubber circuits
Tiny nF cap + small Ω resistor across a switching MOSFET or relay. Watch τ stay under 1 µs to suppress flyback ringing.
Energy harvesting & IoT
Supercap holdover capacitance from 0.1 F to 100 F. Calculate how long a 100 µA load lives off 47 mF at 3.3 V.
Education & coursework
Engineering students see τ, energy, and f_c all together. Drag the curve to scrub time. 63.2% line stays visible.
Vintage radio restoration
Replace failed wax-paper or selenium-era caps with modern equivalents. SMD decoder reads modern markings; presets cover audio coupling values.
Physics lab demos
CGS context shows statfarad and abfarad. A 1 cm vacuum sphere has 1 statF self-capacitance - a true textbook example, live.
Bench debugging
Drop in a 0603 cap labeled 224 - the decoder confirms 220 nF and the schematic re-renders with new plate spacing in under 50 ms.
A short history of capacitance
Capacitance was discovered by accident. In October 1745, the German physicist Ewald Georg von Kleist was experimenting with a nail driven into a small medicine bottle filled with water. He held the bottle in one hand and touched the nail to a friction generator. When he later touched the nail again, the resulting shock knocked him across the room. He had built the world's first capacitor without realising it.
In January 1746 the same effect was independently rediscovered at the University of Leiden by Pieter van Musschenbroek and his student Andreas Cunaeus. Musschenbroek wrote to the French Academy that he "would not take a second shock for the kingdom of France." The device, named the Leyden jar, swept Europe as a parlour curiosity and a scientific tool. Benjamin Franklin used it in 1747 to prove that lightning was electrical, and to coin the terms "positive" and "negative" charge.
The mathematical theory caught up in the 1830s when Michael Faraday introduced the concept of the dielectric: an insulator that stores energy in its electric field. His ratio of charge to voltage - capacitance - laid the groundwork for James Clerk Maxwell's 1860s field theory. The unit was named the farad in 1861, and a sphere of one farad would need a radius larger than the Earth.
Industrial capacitors began with paper-and-foil rolls in the late nineteenth century. The aluminum electrolytic capacitor was invented by the German engineer Charles Pollak in 1896, exploiting the thin oxide layer that grows on aluminum in an electrolyte. This single innovation made microfarad-class capacitors small and cheap, enabling power-supply smoothing, radio tuning, and eventually every consumer electronics circuit.
The next leap came in 1957 when General Electric engineer H. I. Becker patented the electric double-layer capacitor (EDLC), today called a supercapacitor. By exploiting the nanometres-thin charge separation at an electrolyte-electrode interface, supercaps reach farad and kilofarad capacitances in palm-sized packages. They now power memory backup, regenerative braking, and bursts of grid frequency support.
Ceramic multilayer capacitors (MLCCs) took over high-frequency electronics in the 1980s, stacking dozens of dielectric layers under platinum or nickel electrodes. Modern 0402 MLCCs the size of a sesame seed hold 10 µF at 6.3 V. Tantalum and tantalum-polymer caps fill the niche between ceramic and aluminum electrolytic, prized for low ESR and shock tolerance in aerospace and medical gear.
In May 2019, the SI base units were redefined so the elementary charge e equals exactly 1.602176634 × 10⁻¹⁹ coulombs. Because 1 F = 1 C/V and the volt is now traceable to the Planck constant and e, the farad joined the seconds, kilograms, and metres in being defined purely by fundamental constants. Two hundred and seventy-five years after Kleist's electric jolt, the unit that measures stored charge per volt is one of the most precisely defined quantities in physics.
Trusted by RF, power, audio, and academic engineers
“The pF-range RF context with 50 Ω resistor default and live cutoff frequency is exactly what I sketch on paper at every design review. The SMD decoder solved a 0402 mystery I had been chasing for an hour.”
“I drop this on a second monitor while sizing DC-link caps. Switching contexts to Power preselects mΩ ESR-style resistors and mF caps, and the charging curve makes inrush behaviour intuitive for new engineers I mentor.”
“Audio mode with 22 µF coupling and 10 µF crossover presets matches the way I actually order parts. The schematic showing larger plate spacing for bigger caps is gorgeous and makes lectures land for apprentices.”
“My undergrads finally get τ = RC after one minute on this page. Dragging the curve scrubs time, the electrons slow as the cap fills, and the 63.2% line is highlighted. It replaced two lecture slides.”
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