How this Capacitance Converter Works (Formulas & Practical Notes)
This calculator is built to solve everyday capacitor tasks with accuracy and transparency, entirely on the server—no JavaScript required.
At its core, it normalizes any input to farads and then renders human‑readable values across common prefixes. It also computes series/parallel
equivalents, capacitive reactance, RC time constants, stored energy, charge, and tolerance ranges, and it snaps design targets to real‑world
E‑series values for easier part selection.
Unit system and conversion
Capacitance (C) is measured in farads (F). To keep numbers readable, engineers usually work in submultiples. The calculator supports
milifarads (mF), microfarads (µF or uF), nanofarads (nF), picofarads (pF), and femtofarads (fF). Internally, a value like “4.7uF” becomes
4.7 × 10−6 F. Conversions are proportional: Ctarget = CF ÷ scale(target).
| Unit | Symbol | Multiplier to F | Example → F |
| Farad | F | 1 | 1 F → 1 F |
| Milifarad | mF | 10−3 | 3.3 mF → 3.3×10−3 F |
| Microfarad | µF (uF) | 10−6 | 4.7 µF → 4.7×10−6 F |
| Nanofarad | nF | 10−9 | 220 nF → 2.2×10−7 F |
| Picofarad | pF | 10−12 | 1000 pF → 1×10−9 F |
| Femtofarad | fF | 10−15 | 500 fF → 5×10−13 F |
Series, parallel, and real‑world selection
Combining capacitors changes total capacitance. In parallel, capacitances add directly:
Ceq = Σ Ci. In series, reciprocals add:
1/Ceq = Σ (1/Ci). Because real parts are sold in preferred values, the tool also
snaps a target to the nearest E‑series (E6/E12/E24/E96). E‑series are logarithmic sets designed to cover each decade
with roughly constant relative spacing, helping you select parts that are commonly stocked.
| E12 row (one decade) |
| 10, 12, 15, 18, 22, 27, 33, 39, 47, 56, 68, 82 |
Reactance, RC timing, energy, and charge
A capacitor’s opposition to AC is its reactance, |Xc| = 1 / (2π f C) (ohms), which falls as frequency or capacitance increases.
In an RC circuit, the time constant is τ = R·C. After one τ, a step charge reaches about 63.2% of its final value; after five τ, it is above 99%.
Stored energy is E = ½ C V² (joules) and charge is Q = C·V (coulombs).
| Example | Value |
| Given | C = 100 nF, f = 1 kHz, R = 1 kΩ, V = 5 V |
| Reactance | |Xc| ≈ 1 / (2π·1000·100×10−9) ≈ 1.59 kΩ |
| Time constant | τ = R·C = 1000·100×10−9 = 0.0001 s = 0.1 ms |
| Energy | E = ½·C·V² = 0.5·100×10−9·25 ≈ 1.25 µJ |
| Charge | Q = C·V = 100×10−9·5 = 0.5 µC |
Tolerance, temperature, and voltage bias
Real capacitors vary. If tolerance is ±t%, then Cmin = C(1−t) and Cmax = C(1+t).
Because reactance depends on C, your |Xc| and τ will vary accordingly; the calculator shows these ranges.
Multilayer ceramic capacitors (MLCCs) can lose a significant fraction of their capacitance under DC bias, and some dielectrics
(e.g., Y5V) shift with temperature. Use more stable dielectrics (e.g., C0G/NP0 or X7R), derate voltage, and validate at operating
conditions whenever precision matters.
Good design hygiene
Choose values from the relevant E‑series, round thoughtfully, and include margin for tolerance, temperature, and aging.
For filters, look at the full impedance versus frequency; for timing, sanity‑check τ against your clocking and interrupt budgets.
Finally, ensure voltage ratings exceed worst‑case transients, and remember polarized electrolytics are not suitable for AC coupling
unless they are back‑to‑back or specifically designed for bipolar operation.