Design a Capacitor From Bare Geometry
Sometimes the capacitor does not exist yet — it is two pads on a PCB, a sensor plate pair, or a home-built variable cap. Enter the overlapping area, the gap and the material between them, and this calculator solves C = K·ε₀·A/d live, with 25 real dielectric presets and a warning when fringing fields bend the ideal formula.
Parallel Plate Capacitor Calculator
C = K · ε₀ · A / d — geometry in, capacitance out, live on every keystroke.
C = 4.2 × 8.854e-12 × 2.500e-5 m² ÷ 1.600e-3 m
ε₀ = 8.8541878128 × 10⁻¹² F/m. Only the overlapping area counts — offset plates shrink A to their shared region.
Fringing-dominated regime
The plate side (~5 mm, modelled as a square) is under 10× the gap (1.6 mm). Edge fields carry a large share of the charge, so the true capacitance runs above this value — treat the result as a floor.
Anatomy of C = K · ε₀ · A / d
The whole formula fits on one line, and every symbol is a design decision you control. Two plates face each other across a gap; a voltage across them pulls opposite charges onto the plates and the field between stores energy. How much charge accumulates per volt — the capacitance — depends on exactly three things: how much plate faces plate, how far apart they are, and what fills the gap.
Capacitance
What you are solving for, in farads. Real plate geometries land between femtofarads and microfarads — the calculator auto-picks the readable unit from pF upward.
Relative permittivity (dielectric constant)
How much more charge the gap holds with a material between the plates than with vacuum. Air is 1.0005 (effectively vacuum), FR-4 is 4.2, barium titanate reaches thousands. The multiplier lives here.
Vacuum permittivity
8.854 × 10⁻¹² F/m — the constant that converts geometry into capacitance when K = 1. It is why capacitors are small: multiply it by any human-scale area and divide by a human-scale gap and you get picofarads.
Overlapping plate area
The area the two plates share, viewed along the field direction. Only overlap counts: two 10 cm² plates offset so only 3 cm² face each other behave as a 3 cm² capacitor.
Plate separation
The distance between plates, filled with the dielectric. It sits in the denominator, so halving the gap doubles the capacitance — the most powerful knob in the formula and the reason thin dielectrics dominate industry.
The levers are not equally powerful. Area is honest but bulky — doubling it doubles the part. The gap is the aggressive lever: halving d doubles C with no size penalty, which is why the entire capacitor industry has spent a century chasing thinner dielectrics. And K is the multiplier lever, ranging from 1 to over 10 000 between vacuum and exotic ceramics — the difference between a component the size of a coin and one the size of a grain of rice delivering the same microfarads.
ε₀: the Constant That Sets the Scale
Every capacitance calculation starts from an inconveniently small number. The vacuum permittivity, ε₀ = 8.8541878128 × 10⁻¹² F/m, is the proportionality between geometry and charge storage when the gap contains nothing at all. It is not a fudge factor: it is tied to the speed of light through the electromagnetic identity c² = 1/(ε₀µ₀), and no manufacturing cleverness can change it. It is the reason a "huge" 100 mm² plate pair with a 1 mm air gap stores just under a picofarad.
Everything practical in capacitor design is therefore an attack on that number. The dielectric multiplies it by K. Thinning the gap divides by less. Stacking plates adds area. Electrolytics go further still — their "plate" is an etched foil sponge with hundreds of times the geometric area, and their dielectric is an aluminium oxide film a few hundred nanometres thick. The formula never changes; the industry just feeds it better A and d.
The Dielectric Table: 25 Real Materials
The dielectric is where the multiplier lives. The table below lists every material preset the calculator offers, from vacuum (K = 1, the reference) to barium titanate (K ≈ 1200, the ceramic inside your decoupling caps). Where a material's constant varies by grade or formulation, the range is shown. These values are typical published figures for room temperature — always confirm against the specific datasheet when a design depends on precision.
| Material | K (relative permittivity) | Notes |
|---|---|---|
| Vacuum | 1 | Reference / near-reference medium |
| Air (dry, 1 atm) | 1.00054 | Reference / near-reference medium |
| Teflon (PTFE) | 2.1 | |
| Polyethylene | 2.25 | |
| Polystyrene | 2.55 | |
| Polyisobutylene | 2.2 | |
| Mineral oil | 2.23 | |
| Kraft paper | 2.6 | |
| Polycarbonate | 3.1 | |
| Paper (waxed) | 3.5 | |
| Silicon dioxide (SiO₂) | 3.7 | |
| FR-4 (PCB substrate) | 4.2 | |
| Concrete | 4.5 | |
| Glass | 4.7 (3.7–10) | |
| Ruby mica | 7.5 (6.5–8.7) | |
| Rubber (hard) | 7 | |
| Aluminium oxide (Al₂O₃) | 8.4 | |
| Silicon | 11.68 | |
| Tantalum pentoxide (Ta₂O₅) | 28 | |
| Methanol | 30 | |
| Niobium oxide | 40 | |
| Titanium dioxide (TiO₂) | 80 | |
| Water (20 °C) | 80.1 | |
| Strontium titanate | 310 | High-K family — value drifts with voltage and temperature |
| Barium titanate (Class 2) | 1200 (200–12 000) | High-K family — value drifts with voltage and temperature |
Reading the table strategically: the bottom third (K ≥ 100) buys capacitance at the cost of stability — those materials lose value under DC bias and wander with temperature, which is acceptable for decoupling and fatal for timing. The middle band (K ≈ 4–9) is the precision sweet spot: FR-4, glass, mica and aluminium oxide pair respectable multipliers with stable behaviour. The top of the table barely multiplies at all but never lies — vacuum, air and PTFE are the dielectrics of metrology, RF and anything that must not drift.
Fringing Fields: Where the Ideal Formula Bends
C = K·ε₀·A/d assumes the electric field is a clean, uniform column between the plates that simply stops at the edges. Real fields bulge outward around every rim, wrapping the edges in extra field lines that store extra charge — capacitance the formula never counts. The size of that error depends on one geometric ratio: how the plate side length compares to the gap. The calculator models your plates as a square of side √A and flags the regime automatically.
Ideal
Edge effects are negligible and C = K·ε₀·A/d is accurate to well under 1%. Design in this regime whenever space allows — most PCB and sensor geometry lands here naturally.
Mild fringing
The field bulges slightly outward and the true capacitance runs a few percent above the formula. Fine for decoupling and general work; add margin if the value feeds a timing or tuned circuit.
Fringing-dominated
Edge fields carry a large share of the charge and the ideal formula understates capacitance by 10% or more, increasingly so as the ratio shrinks. The calculator flags this regime — treat its result as a floor, not a value.
Two corollaries are worth internalising. First, tiny sensors are fringing machines: a capacitive touch pad or MEMS comb drive operates deliberately in the fringing regime because the edge fields are precisely what a fingertip or moving tooth modulates. Their designs use corrected field models, not the schoolbook formula. Second, partial fills break the formula a second way: if the dielectric occupies only part of the gap, the capacitor becomes two capacitors in series (material and air), and the effective K drops below either — which is exactly how capacitive liquid-level sensors work.
The practical habit: prefer designs with plate sides at least 50× the gap when the computed value feeds a tuned or timing circuit, and treat anything below 10× as an estimate to verify on a meter.
Three Designs the Formula Actually Solves
The same five symbols describe a parasitic on a PCB, a knob-controlled radio part and the die inside a decoupling cap. These three worked cases cover the range — run each one through the calculator above to see the units flow.
Two PCB pads across FR-4
A = 25 mm², d = 1.6 mm (FR-4 core), K = 4.2
C ≈ 0.58 pF
This is real parasitic capacitance: two default-sized pads on opposite sides of a standard 1.6 mm board carry over half a picofarad — enough to matter in RF layouts and capacitive sensing.
Home-built air variable capacitor
A = 100 cm², d = 1 mm, K = 1.0005 (air)
C ≈ 88.6 pF
A classic hobby construction: interleaved aluminium plates with a 1 mm air gap sweep tens to hundreds of picofarads as the overlap changes — sliding the A term of the formula by hand.
Class 2 ceramic inside a 0805 package
A ≈ 1 mm², d ≈ 10 µm, K = 1200 (barium titanate)
C ≈ 0.106 µF
Shrink everything and let the dielectric do the work: a grain of barium titanate ten microns thick yields a tenth of a microfarad from a chip the size of a Pinhead. Thin d plus huge K is the entire industry in one line of arithmetic.
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Open calculatorPlate Capacitor FAQ
How do I calculate capacitance from plate area and separation?▼
Use C = K × ε₀ × A / d: multiply the dielectric constant by the vacuum permittivity (8.854 × 10⁻¹² F/m) and the overlapping plate area in square metres, then divide by the plate separation in metres. For example, two 25 mm² plates on opposite sides of 1.6 mm FR-4 give 4.2 × 8.854×10⁻¹² × 25×10⁻⁶ ÷ 1.6×10⁻³ ≈ 0.58 pF. The calculator above performs the conversion from mm², cm², m², sq in or sq ft, and from µm, mm, cm, m, mil or inches, so only the numbers themselves need to be entered.
What is ε₀ and why does it appear in the formula?▼
ε₀ is the vacuum permittivity: 8.8541878128 × 10⁻¹² farads per metre. It is the proportionality constant that converts geometry (area divided by gap) into capacitance when the gap is empty space. Every material multiplies it by its relative permittivity K. The number is not arbitrary — it falls out of the speed of light and the magnetic constant (c² = 1/ε₀µ₀) — which is why no amount of geometry cleverness escapes it: vacuum capacitor designs all inherit the same tiny base value.
Which dielectric gives the most capacitance?▼
Barium titanate, by a wide margin: K ≈ 1200 for Class 2 formulations, with some compositions reaching into the thousands. It is the ceramic inside common MLCC decoupling capacitors. The practical trade-offs are voltage and precision — high-K ceramics lose capacitance under DC bias, drift with temperature, and carry loose tolerances (Z-band in extreme cases). For stable values, lower-K materials win: C0G/NP0 ceramics (K ≈ 20–100), film (≈ 2–3) and mica (≈ 7) hold their value across voltage, temperature and time.
Water has K ≈ 80 — why don't we build capacitors with it?▼
Because high K is not the only requirement. Water is a polar molecule: it conducts impurities readily, electrolyses under DC bias, freezes at 0 °C, boils at 100 °C, and its permittivity collapses above a few GHz. A water-dielectric capacitor leaks, corrodes its plates and changes value with every degree. The lesson generalises: the K column of the table is a starting point, and usable dielectrics must also hold off voltage, stay stable and refuse to conduct — which is why ceramics, polymers and oxides dominate.
When is the parallel-plate formula wrong?▼
Chiefly in the fringing regime. The formula assumes the field between the plates is uniform and simply ends at the plate edges; in reality it bulges outward, adding edge capacitance the formula never counts. When the plate dimensions are at least 50× the gap, the error is negligible. Below about 10× the gap, the error grows past 10% and the calculator's result becomes a floor rather than a value. The formula also assumes the dielectric fills the gap completely — an air bubble or partial fill creates a series combination of two capacitors, not one clean value.
How do I convert my dimensions into the calculator's units?▼
You do not have to — enter area in mm², cm², m², square inches or square feet, and separation in µm, mm, cm, m, mils or inches, picking from the dropdown beside each field. For reference: 1 sq in = 645.16 mm², 1 mil = 25.4 µm, and a US 0603 pad pair overlaps roughly 0.5 mm². Once the value is computed, the result is quoted in auto-picked units from pF upward; if you need it in a specific unit, the capacitance converter page translates pF, nF, µF, mF and F in one step.
Can I stack multiple plate capacitors to get more?▼
Yes — and the stacking rule depends on how you wire it. N identical plate capacitors wired in parallel add directly (N × C), which is exactly what a multi-plate air variable capacitor does by interleaving plates: every adjacent pair is one parallel contribution. Wired in series, N equal capacitors give C/N with N-fold voltage rating — useful for high-voltage probes, at the cost of value. The series & parallel calculator handles both combinations for up to 12 arbitrary values, including mixed units.
What capacitance can real PCB geometry achieve?▼
More than intuition suggests, less than a component does. Two default pads across a 1.6 mm FR-4 core: ~0.6 pF. Wide traces over a ground plane in a 4-layer stack (gap 0.2 mm): several pF per centimetre of run. An interleaved interdigitated comb structure can reach tens of pF in a few square millimetres. That range — fractions of a pF to tens of pF — is exactly why board-level parasitics matter for RF and sensing and are ignorable for digital decoupling. Compute your own geometry above before trusting a layout rule of thumb.
Two Dimensions and a Material Away
Pick a dielectric from the table, type the area and the gap, and the capacitance is on screen before the soldering iron warms up.