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Capacitor - Geometry and Charge Storage

Capacitance depends on geometry: parallel plate C = ε₀εrA/d, cylindrical and spherical have different formulas. Charge Q = CV, energy E = ½CV². Reactance Xc = 1/(2πfC) for AC.

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Parallel plate C proportional to area, inversely to separation Dielectric εr increases capacitance by factor of εr Cylindrical and spherical have different geometry factors Reactance Xc decreases with frequency

Key quantities
ε₀εrA/d
C (plate)
Key relation
CV
Q
Key relation
½CV²
E
Key relation
1/(2πfC)
Xc
Key relation

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Why: Capacitors store energy in electric fields. Geometry determines capacitance—parallel plates, cylinders, and spheres have different formulas. Essential for circuit design, filters, and energy storage.

How: Parallel plate: C = ε₀εrA/d. Cylindrical: C = 2πε₀εrL/ln(b/a). Spherical: C = 4πε₀εrab/(b-a). Charge Q = CV. Energy E = ½CV² = ½QV.

Parallel plate C proportional to area, inversely to separationDielectric εr increases capacitance by factor of εr

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Calculate Capacitor ParametersSelect geometry and enter dimensions to find capacitance, charge, or energy.

⚙️ Capacitor Parameters

Area (A)

Plate area

📚 What is a Capacitor?

A capacitor is a passive electronic component that stores electrical energy in an electric field. It consists of two conductive plates separated by a dielectric (insulating) material.

C = ε₀εᵣA/d

Where C is capacitance (Farads), ε₀ is vacuum permittivity (8.854×10⁻¹² F/m), εᵣ is relative permittivity, A is plate area (m²), and d is plate separation (m).

Capacitors are fundamental components in electronics, used for energy storage, filtering, timing circuits, power factor correction, and signal coupling.

📐 Key Formulas

Capacitance Formulas

Parallel Plate: C = ε₀εᵣA/d

Cylindrical: C = 2πε₀εᵣL/ln(r₂/r₁)

Spherical: C = 4πε₀εᵣr₁r₂/(r₂-r₁)

Charge & Energy

Charge: Q = CV

Energy: E = ½CV² = Q²/(2C)

Energy Density: u = ½εE²

AC Behavior

Reactance: Xc = 1/(2πfC)

Impedance: Z = -jXc

Phase: Current leads voltage by 90°

RC Circuits

Time Constant: τ = RC

Charging: V(t) = V₀(1-e^(-t/τ))

Discharging: V(t) = V₀e^(-t/τ)

🔧 How Capacitors Work

Energy Storage: When voltage is applied, electrons accumulate on one plate and are removed from the other, creating an electric field. The energy stored is proportional to the square of the voltage.

DC Behavior: Capacitors block DC current once charged. They act as open circuits in steady-state DC circuits.

AC Behavior: Capacitors allow AC current to pass, with reactance inversely proportional to frequency. Higher frequencies see lower reactance.

Charging/Discharging: In RC circuits, capacitors charge and discharge exponentially with time constant τ = RC. After 5τ, the capacitor is essentially fully charged/discharged.

Dielectric Effect: Dielectric materials increase capacitance by reducing the electric field between plates. The relative permittivity (εᵣ) determines the increase factor.

When to Use Capacitors

Timing Circuits

RC circuits use capacitors for delays, oscillators, and pulse generation. Time constant τ = RC determines timing.

Filtering

Low-pass filters block high frequencies. High-pass filters block DC. Band-pass filters combine both.

Power Factor Correction

Capacitors compensate for inductive loads, improving power factor and reducing utility penalties.

Energy Storage

Supercapacitors store energy for backup power, regenerative braking, and peak power delivery.

Coupling/Decoupling

AC coupling capacitors pass signals while blocking DC. Decoupling capacitors filter power supply noise.

Tuning Circuits

LC resonant circuits use capacitors with inductors for frequency selection in radios and oscillators.

📊 Sample Examples

Example 1: Timing Circuit (555 Timer)

A 555 timer uses R = 10 kΩ and C = 10 µF. Calculate the time constant and pulse width.

Solution: τ = RC = 10,000 × 10×10⁻⁶ = 0.1 s = 100 ms. Pulse width ≈ 1.1τ = 110 ms.

Example 2: Low-Pass Filter Design

Design a low-pass filter with cutoff frequency 1 kHz using C = 0.1 µF. Find required resistance.

Solution: f_c = 1/(2πRC) → R = 1/(2πf_cC) = 1/(2π × 1000 × 0.1×10⁻⁶) = 1,591 Ω ≈ 1.6 kΩ

Example 3: Energy Storage

A 1000 µF capacitor charged to 400 V stores how much energy?

Solution: E = ½CV² = ½ × 1000×10⁻⁶ × 400² = 0.5 × 0.001 × 160,000 = 80 J

Example 4: Power Factor Correction

A motor needs 53 Ω capacitive reactance at 50 Hz for PF correction. What capacitor value?

Solution: Xc = 1/(2πfC) → C = 1/(2πfXc) = 1/(2π × 50 × 53) = 60 µF

Example 5: Audio Coupling

An audio amplifier needs AC coupling with Xc = 159 Ω at 20 Hz. Calculate capacitor value.

Solution: C = 1/(2πfXc) = 1/(2π × 20 × 159) = 50 µF

🌐 Capacitor Geometries

Parallel Plate

Most common geometry. C = ε₀εᵣA/d

Used in: Standard capacitors, variable capacitors, MEMS devices

Cylindrical

Coaxial design. C = 2πε₀εᵣL/ln(r₂/r₁)

Used in: Coaxial cables, high-voltage capacitors, RF applications

Spherical

Concentric spheres. C = 4πε₀εᵣr₁r₂/(r₂-r₁)

Used in: High-voltage applications, theoretical models, Van de Graaff generators

🔬 Dielectric Materials

MaterialεᵣBreakdown (V/µm)Applications
Vacuum1.0-Reference
Air1.00063Variable capacitors
Paper2-415-20Old capacitors
Mica5-7100-200High-frequency
Ceramic10-10,00010-100General purpose
Tantalum~27~50Small size, stable
Aluminum Oxide~9~600Electrolytic

Frequently Asked Questions

Why does energy scale with V²?

Energy is the integral of charge times voltage. Since Q = CV, and we integrate from 0 to V, we get E = ½CV². The ½ factor comes from the linear charging process.

Why do capacitors block DC?

Once charged, a capacitor's plates have equal and opposite charges. No net current flows because the electric field prevents further charge movement. DC sees infinite impedance.

What happens at high frequencies?

Reactance Xc = 1/(2πfC) decreases with frequency. At very high frequencies, capacitors act like short circuits, passing AC signals easily.

Can capacitors store energy forever?

No. Real capacitors have leakage resistance that slowly discharges them. Supercapacitors can hold charge for days, but eventually self-discharge.

Why are capacitors in parallel additive?

Parallel capacitors share the same voltage but store separate charges. Total charge Q_total = Q₁ + Q₂ = C₁V + C₂V = (C₁ + C₂)V, so C_total = C₁ + C₂.

Why are capacitors in series like resistors in parallel?

Series capacitors share the same charge but have different voltages. V_total = V₁ + V₂ = Q/C₁ + Q/C₂ = Q(1/C₁ + 1/C₂), so 1/C_total = 1/C₁ + 1/C₂.

📚 Official Data Sources

NIST Physics

Physical constants and standard reference data

HyperPhysics - Capacitors

Capacitor physics and formulas

Electronics Tutorials

Capacitor theory and applications

Khan Academy - Circuits

Circuit analysis and capacitor behavior

All About Circuits

Comprehensive electronics education

⚠️ Disclaimer

This calculator is for educational and design purposes. Real capacitors have parasitic effects (ESR, ESL, leakage) that may affect performance. For critical applications in power electronics, RF circuits, or safety systems, consult manufacturer datasheets and verify calculations with experimental testing. Always follow proper safety procedures when working with charged capacitors.

For educational and informational purposes only. Verify with a qualified professional.

🔬 Physics Facts

Parallel plate capacitance C = ε₀εrA/d; ε₀ = 8.854×10⁻¹² F/m

— HyperPhysics

📐

Cylindrical capacitors used in coaxial cables; C = 2πεL/ln(b/a)

— NIST

💾

Spherical capacitor formula C = 4πε₀ab/(b-a) for concentric spheres

— Khan Academy

📊

Dielectric constant εr of water ~80; air ~1; ceramics 100-10000

— NIST

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