🔋 Capacitance Conversion Calculator
Convert between pF, nF, µF, mF, F, kF and 20+ capacitance units — with circuit formulas & capacitor markings guide
🔄 Capacitance Unit Converter
📊 All Conversions at Once
📖 How to Use the Capacitance Converter
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1Enter Your Capacitance Value
Type the numerical capacitance value into the "Enter Value" field. Decimals and scientific notation are supported (e.g., 4.7e-9 for 4.7 nF). Results update instantly as you type.
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2Select the Source Unit (From)
Choose your input unit from the "From Unit" dropdown — from picofarad (pF) to terafarad (TF), including special units such as abfarad and statfarad.
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3Select the Target Unit (To)
Choose the unit you want to convert into from the "To Unit" dropdown. The result and the exact multiplication factor appear immediately in the result panel.
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4Use Quick-Convert Buttons
Click a quick-convert button (nF→pF, µF→nF, etc.) for the most common conversions — the dropdowns are pre-set and the result is calculated instantly.
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5View All Conversions & Copy
The "All Conversions at Once" panel shows your value in every supported unit simultaneously. Click "📋 Copy Result" to copy the primary result to your clipboard.
📐 Capacitance Units Reference Table
| Unit | Symbol | Value in Farads | Math Expression | Common Use |
|---|---|---|---|---|
| Picofarad | pF | \(10^{-12}\,\text{F}\) | \( 1\,\text{pF} = 10^{-12}\,\text{F} \) | RF circuits, ceramic caps, sensors |
| Nanofarad | nF | \(10^{-9}\,\text{F}\) | \( 1\,\text{nF} = 10^{-9}\,\text{F} \) | Timing, signal coupling, filters |
| Microfarad | µF | \(10^{-6}\,\text{F}\) | \( 1\,\mu\text{F} = 10^{-6}\,\text{F} \) | Power supply filtering, audio |
| Millifarad | mF | \(10^{-3}\,\text{F}\) | \( 1\,\text{mF} = 10^{-3}\,\text{F} \) | Large electrolytic caps |
| Farad (SI base) | F | \(1\,\text{F}\) | \( 1\,\text{F} = 1\,\text{C/V} \) | Supercapacitors, energy storage |
| Kilofarad | kF | \(10^{3}\,\text{F}\) | \( 1\,\text{kF} = 1000\,\text{F} \) | Large supercapacitors, EDLC banks |
| Abfarad | abF | \(10^{9}\,\text{F}\) | \( 1\,\text{abF} = 10^9\,\text{F} \) | CGS-EMU (historical) |
| Statfarad | statF | \(\approx 1.1127 \times 10^{-12}\,\text{F}\) | \( 1\,\text{statF} = \frac{1}{c^2} \times 10^{11}\,\text{F} \) | CGS-ESU / Gaussian (theoretical) |
🔬 Understanding Capacitance — A Complete Guide
Capacitance is the ability of a component or system to store electric charge for a given voltage difference across it. It is one of the three fundamental passive electrical properties — alongside resistance and inductance — that determine the behaviour of all electronic circuits. From the 22 pF trimmer capacitor tuning a radio receiver, to the 100 µF electrolytic capacitor smoothing a power supply, to the 3,000 F supercapacitor storing regenerative braking energy in a hybrid vehicle, capacitance spans more than 15 orders of magnitude in engineering practice.
The SI unit of capacitance is the farad (F), named after the English scientist Michael Faraday (1791–1867), whose pioneering experiments with electrochemical cells and electromagnetic induction laid the foundations of modern electrical engineering. The farad is defined as the capacitance of a capacitor that stores exactly one coulomb of charge when a potential difference of one volt is applied across its terminals.
This deceptively simple equation encapsulates the entire physics of capacitance. A larger capacitance stores more charge for the same applied voltage; a smaller capacitance stores less. Because the farad is an extremely large unit relative to typical component values — a 1 F capacitor at 1 V stores 1 coulomb, which represents \(6.24 \times 10^{18}\) electron charges — virtually all practical capacitors are measured in fractions of a farad: microfarads (µF), nanofarads (nF), or picofarads (pF).
🔢 pF, nF, µF — The Prefix Scale Explained
The three most commonly encountered capacitance units form a factor-of-1,000 ladder. Understanding these relationships is essential for reading component datasheets, interpreting capacitor markings, and designing circuits correctly:
Picofarad (pF) — \(10^{-12}\,\text{F}\)
The smallest commonly used unit. Typical range: 1 pF to 10,000 pF. Used in RF and microwave circuits, ceramic capacitors, variable trimmer caps, crystal load capacitors, antenna matching networks, and parasitic-capacitance analysis on PCBs.
Nanofarad (nF) — \(10^{-9}\,\text{F}\)
Middle of the practical range. 1 nF = 1,000 pF = 0.001 µF. Common for ceramic and film capacitors in signal filters, timing circuits (RC timers), audio coupling, EMI suppression, and decoupling on digital logic supplies.
Microfarad (µF) — \(10^{-6}\,\text{F}\)
The workhorse of power electronics. 1 µF = 1,000 nF = 1,000,000 pF. Electrolytic and tantalum capacitors in power supply filtering, motor start/run capacitors (2–30 µF), audio amplifier coupling and bypass (>10 µF).
Farad (F) & Above — Supercapacitors
Electric double-layer capacitors (EDLC) and pseudocapacitors reach 1 F to 10,000 F. Used for energy storage, UPS hold-up, regenerative braking, engine cold-start assist, and replacing batteries in low-power IoT devices.
⚡ The Physics of a Capacitor
Parallel Plate Capacitor
The simplest physical model of a capacitor is two parallel conducting plates separated by a dielectric (insulating) material. The capacitance is determined by the plate geometry and the dielectric properties:
This formula explains the design choices in capacitor manufacturing:
- Larger plate area A → higher capacitance. Electrolytic capacitors use a chemically etched aluminium foil to dramatically increase effective surface area.
- Smaller separation d → higher capacitance. The oxide layer in electrolytic capacitors is nanometres thin — far thinner than any physically cut insulator.
- Higher permittivity \(\varepsilon_r\) → higher capacitance. Ceramic capacitors use materials with \(\varepsilon_r\) as high as 20,000 (Class II X7R, Y5V) vs. 1 for vacuum.
Given: Two square plates, 10 cm × 10 cm (A = 0.01 m²), separated by 0.1 mm = \(10^{-4}\) m of polyethylene (\(\varepsilon_r = 2.3\)).
\[ C = 8.854 \times 10^{-12} \times 2.3 \times \frac{0.01}{10^{-4}} = 8.854 \times 10^{-12} \times 2.3 \times 100 \]
\[ C \approx 2.037 \times 10^{-9}\,\text{F} = 2.037\,\text{nF} = 2,037\,\text{pF} \]
Answer: Approximately 2.0 nF — well within the nanofarad range for a palm-sized film capacitor.
🔋 Energy Stored in a Capacitor
A charged capacitor stores electrical energy in the electric field between its plates. The energy is given by:
Given: A camera flash capacitor C = 1,000 µF = 0.001 F charged to V = 300 V.
\[ E = \frac{1}{2} \times 0.001 \times (300)^2 = \frac{1}{2} \times 0.001 \times 90{,}000 = 45\,\text{J} \]
Answer: The capacitor stores 45 joules — enough to produce an intense flash lasting a few milliseconds. This is why charged camera flash capacitors are dangerous even after the camera is off.
Given: A supercapacitor rated C = 3,000 F charged to V = 2.7 V (its rated voltage).
\[ E = \frac{1}{2} \times 3{,}000 \times (2.7)^2 = \frac{1}{2} \times 3{,}000 \times 7.29 = 10{,}935\,\text{J} \approx 3.04\,\text{Wh} \]
Answer: The supercapacitor stores approximately 3 Wh — usable for engine start-stop assist or backup power for IoT sensors.
⏱️ RC Time Constant — Charge and Discharge
When a capacitor is connected to a resistor and a voltage source, it does not charge or discharge instantaneously — it follows an exponential curve governed by the RC time constant \(\tau\) (tau):
The voltage across the capacitor during charging is: \[ V_C(t) = V_s \left(1 - e^{-t/\tau}\right) \] And during discharging: \[ V_C(t) = V_0 \, e^{-t/\tau} \] where \(V_s\) is the supply voltage, \(V_0\) is the initial voltage, and \(e \approx 2.718\) is Euler's number.
Given: A 555 timer circuit with R = 10 kΩ and C = 100 nF = \(10^{-7}\) F.
\[ \tau = R \times C = 10{,}000 \times 10^{-7} = 10^{-3}\,\text{s} = 1\,\text{ms} \]
The oscillation frequency in astable mode (with R1 = R2 = 10 kΩ, C = 100 nF) is approximately:
\[ f \approx \frac{1.44}{(R_1 + 2R_2) \times C} = \frac{1.44}{30{,}000 \times 10^{-7}} \approx 480\,\text{Hz} \]
Answer: The timer generates a square wave at approximately 480 Hz — audible as a buzzing tone.
📡 Capacitive Reactance — AC Circuit Behaviour
In AC circuits, a capacitor offers a frequency-dependent opposition to current flow called capacitive reactance \(X_C\). Unlike resistance, reactance is not constant — it decreases as frequency increases, meaning capacitors pass high-frequency signals more easily than low-frequency ones. This is the fundamental principle behind capacitive filtering and bypass circuits.
Given: A 100 nF decoupling capacitor on a 5 V logic rail. Find its reactance at 1 MHz and at 100 MHz.
At 1 MHz: \( X_C = \dfrac{1}{2\pi \times 10^6 \times 10^{-7}} = \dfrac{1}{0.6283} \approx 1.59\,\Omega \)
At 100 MHz: \( X_C = \dfrac{1}{2\pi \times 10^8 \times 10^{-7}} = \dfrac{1}{62.83} \approx 0.0159\,\Omega \)
Answer: At 1 MHz it presents 1.59 Ω — adequately low for decoupling. At 100 MHz, 15.9 mΩ, effectively a short circuit to noise.
🔗 Capacitors in Series and Parallel
Two 10 µF capacitors in parallel: \( C = 10 + 10 = 20\,\mu\text{F} \)
Two 10 µF capacitors in series: \( \frac{1}{C} = \frac{1}{10} + \frac{1}{10} = \frac{2}{10} \Rightarrow C = 5\,\mu\text{F} \)
Note: For two identical capacitors C in series the result is always C/2. This is useful when you need a lower-rated capacitor value that isn't in stock: two 10 µF → 5 µF.
🏷️ How to Read Capacitor Markings
Most ceramic and film capacitors are marked with a three-digit code that indicates capacitance in picofarads. Understanding this code avoids costly errors when identifying or sourcing components.
- The first two digits are the significant figures
- The third digit is the number of zeros to append (the multiplier exponent)
- The value is always in picofarads (pF)
| Code | Calculation | Value (pF) | Value (nF) | Value (µF) |
|---|---|---|---|---|
| 100 | \(10 \times 10^0 = 10\) | 10 pF | 0.010 nF | 0.000010 µF |
| 101 | \(10 \times 10^1 = 100\) | 100 pF | 0.10 nF | 0.000100 µF |
| 102 | \(10 \times 10^2 = 1{,}000\) | 1,000 pF | 1.0 nF | 0.001 µF |
| 103 | \(10 \times 10^3 = 10{,}000\) | 10,000 pF | 10 nF | 0.01 µF |
| 104 | \(10 \times 10^4 = 100{,}000\) | 100,000 pF | 100 nF | 0.1 µF |
| 105 | \(10 \times 10^5 = 1{,}000{,}000\) | 1,000,000 pF | 1,000 nF | 1 µF |
| 474 | \(47 \times 10^4 = 470{,}000\) | 470,000 pF | 470 nF | 0.47 µF |
| 223 | \(22 \times 10^3 = 22{,}000\) | 22,000 pF | 22 nF | 0.022 µF |
🔌 Types of Capacitors and Their Typical Values
| Type | Typical Range | Voltage Rating | Key Properties |
|---|---|---|---|
| Ceramic (Class I — C0G/NP0) | 1 pF – 1 µF | 50 V – 5 kV | Low loss, stable with T, precise; ideal for RF and timing |
| Ceramic (Class II — X7R, X5R) | 1 nF – 100 µF | 6.3 V – 100 V | High capacitance density; C varies with voltage and temperature |
| Ceramic (Class III — Y5V, Z5U) | 1 nF – 100 µF | Up to 50 V | Highest density; wide C tolerance (−20%/+80%); poor stability |
| Aluminium Electrolytic | 1 µF – 100,000 µF | 6.3 V – 500 V | Polarised; large capacitance; ESR limits HF performance; limited life |
| Tantalum Electrolytic | 0.1 µF – 2,200 µF | 4 V – 63 V | Stable; low ESR; sensitive to overvoltage; can ignite if reverse-biased |
| Film (Polyester / PET) | 1 nF – 100 µF | 50 V – 600 V | Non-polarised; stable; low cost; audio-grade; motor run use |
| Film (Polypropylene / PP) | 100 pF – 50 µF | 250 V – 2 kV | Lowest loss; excellent RF/audio; pulse power; EMI suppression X2 |
| Supercapacitor (EDLC) | 0.1 F – 10,000 F | 2.5 V – 3.0 V | Enormous capacitance; 1 million cycle life; low voltage; energy storage |
| Mica | 1 pF – 10,000 pF | 100 V – 1 kV | Ultra-stable; low loss; precision; used in RF tank and filter circuits |