Capacitance Calculator
Compute capacitance for common geometries (parallel-plate, coaxial/cylindrical, spherical), series/parallel combinations, and the energy stored in a capacitor. Supports unit conversions (pF, nF, μF, mF, F) and step-by-step derivations.
Parallel-plate: C = ε₀ ε_r A / d
Coaxial cylinders: C' = 2π ε₀ ε_r / ln(b/a) (per unit length)
Spherical capacitor: C = 4π ε₀ ε_r (ab)/(b - a) for concentric spheres
Series and Parallel: combine capacitors
Energy & charge: U = ½ C V² ; Q = C V
Capacitance: fundamentals, formulas and practical considerations
Capacitance measures a system's ability to store electric charge. A capacitor stores equal and opposite charges on two conductors separated by a dielectric. The basic definition is C = Q / V, where Q is charge and V potential difference. The SI unit is the farad (F), but typical capacitors use microfarads (μF), nanofarads (nF) or picofarads (pF).
Common capacitor geometries
Parallel-plate capacitor: two plates of area A separated by distance d with dielectric ε = ε₀ ε_r give C = ε₀ ε_r A / d. This is the simplest and widely used for deriving scaling laws: capacitance grows with area and dielectric constant, and decreases with separation.
Coaxial (cylindrical) capacitor: two concentric cylinders of radii a (inner) and b (outer) and length L (≫ radii) have capacitance C = (2π ε₀ ε_r L) / ln(b/a). The formula is often written per unit length: C' = 2π ε₀ ε_r / ln(b/a).
Spherical capacitor: two concentric spheres with radii a and b have C = 4π ε₀ ε_r (ab)/(b - a). In the limit b → ∞ (isolated sphere), the self-capacitance tends to 4π ε₀ ε_r a.
Series and parallel combinations
Capacitors in parallel add directly: C_eq = Σ C_i. Series follows 1/C_eq = Σ 1/C_i, the opposite of resistors. This behaviour comes from how voltage and charge distribute in each configuration.
Energy storage
The energy stored in a capacitor is U = ½ C V². This formula is derived by integrating the work required to move incremental charge onto the capacitor while raising its voltage. For fixed charge, U = Q²/(2C).
Dielectrics and practical notes
Dielectrics increase capacitance by a factor ε_r. Real dielectrics also introduce losses (dielectric loss tangent), breakdown strength (maximum field before breakdown), and temperature dependence. For high-voltage or precision capacitors, geometry, surface finish, and connecting leads (fringe fields) matter.
Worked examples
Example 1 — Parallel-plate. Two square plates 10 cm × 10 cm (A=0.01 m²), separated by 1 mm (d=0.001 m) in air (ε_r ≈ 1). C = ε₀ A / d ≈ (8.854e-12 × 0.01) / 0.001 = 8.854e-13 / 0.001 = 8.85e-11 F = 88.5 pF.
Example 2 — Coaxial cable. Inner radius a = 0.5 mm, outer b = 2.5 mm, ε_r = 2.2 (typical dielectric), L = 1 m. C = 2π ε₀ ε_r L / ln(b/a). Compute ln(5)=1.609, so C ≈ (2π × 8.85e-12 × 2.2 × 1)/1.609 ≈ 7.6e-11 F ≈ 76 pF/m.
Limitations and design tips
- Use correct units — converting mm² to m² or pF to F is a common error.
- For small separations, edge effects become important; finite-element simulation may be required for accurate values.
- Keep dielectric thickness uniform and avoid sharp edges which concentrate electric field and cause breakdown.
When to use this calculator
Use the formulas here for classroom problems, quick design checks, and sanity checks on measurements. For detailed engineering of high-voltage capacitors, consult specialized design procedures and standards.
Frequently Asked Questions
Use ε₀ = 8.8541878128×10⁻¹² F/m (commonly 8.854e-12 F/m).
1 μF = 1×10⁻⁶ F. Similarly, 1 nF = 1×10⁻⁹ F; 1 pF = 1×10⁻¹² F.
Only when plate dimensions are large compared to separation; otherwise include fringing corrections or simulate numerically.
In series the same charge sits on all capacitors but voltages add, so equivalent capacitance decreases.
Use the coaxial formula per unit length: C' = 2π ε₀ ε_r / ln(b/a) and multiply by length.
Unintended capacitance between components or traces; it can affect high-frequency circuits and must be minimized where necessary.
Use numerical methods (FEM) or approximate by decomposing shapes into known geometries.
Yes — dielectric constants and geometry (thermal expansion) can change capacitance slightly with temperature; special capacitors minimize this drift.
Yes conceptually (C = Q/V), but supercapacitors use electrochemical double layers producing very high capacitance per volume and require careful handling.
Classroom problems, rough design, cable capacitance estimates, and energy storage checks for simple capacitor geometries.