A capacitor is a two-terminal passive electrical device that stores energy in the form of an electric field. It is widely used in electronic circuits for storing energy temporarily, filtering signals, and managing timing operations.
The charge stored in a capacitor is directly proportional to the voltage across its plates:
q ∝ V → q = CV
Where:
Capacitance refers to the capacity of a capacitor to hold electric charge in relation to the applied voltage:
C = q / V
Its SI unit is the Farad (F), where:
1 F = 1 Coulomb/Volt
Since 1 Farad is very large, practical capacitors are usually measured in microfarads (μF), nanofarads (nF), or picofarads (pF).
The electric field E between the plates of a parallel plate capacitor is given by:
E = V / d = σ / (ε0εr) = q / (A ε0 εr)
Where:
Using C = q / V and substituting from the electric field expression:
C = ε0εr A / d
If the space between the plates is vacuum or air (εr = 1), then:
C = ε0 A / d
For capacitors with layered dielectrics of varying thickness, the effective capacitance is:
C = ε0 A / (Z·d / εr)
Where Z·d / εr represents the effective dielectric-adjusted thickness.
For capacitors with n plates connected alternately, the equivalent capacitance becomes:
C = (n − 1) ε0 εr A / d
For an isolated spherical conductor of radius r in a medium with permittivity εr, the potential is:
V = q / (4π εr r)
Therefore, the capacitance is:
C = q / V = 4π εr r
Hence, capacitance is directly proportional to the radius:
C ∝ r
Understanding these fundamental equations and their derivations is essential for mastering capacitor-related problems. Practice numerical applications of these formulas to build a strong conceptual foundation.