Parallel plate capacitors
Physical properties of a parallel plate capacitor
A parallel plate capacitor consists of two separated parallel conducting surfaces that can hold equal amounts of charge with opposite signs.
Capacitance (\(C\)) relates the magnitude of the charge stored on each plate to the electric potential difference created by the separation of those charges. \[\begin{equation} C = \dfrac{Q}{\Delta V}. \end{equation}\] It is measured in farads, where \(\qty{1}{\farad} = \qty{1}{\coulomb\per\volt}\). In practice, a farad is a large unit; the ones you typically might see in electronics lab range in the pF to μF range.
The capacitance of a capacitor depends only on the physical properties of the capacitor, such as the capacitor’s shape, geometry, and the material used to separate the plates.
The capacitance of a parallel-plate capacitor is proportional to the area of one of its plates and inversely proportional to the distance between its plates. The constant of proportionality is the product of the dielectric constant, \(\kappa\) , of the material between the plates and the electric permittivity of free space, \(\epsilon_0\). \[\begin{equation} C = \dfrac{\kappa \epsilon_0 A}{d} \end{equation}\]
The electric field between two charged parallel plates with uniformly distributed electric charge, such as in a parallel-plate capacitor, is constant in both magnitude and direction, except near the edges of the plates. The magnitude of the electric field between two charged parallel plates, where the plate separation is much smaller than the dimensions of the plates, can be determined by applying Gauss’s law and the principle of superposition. \[\begin{equation} E = \dfrac{Q}{\epsilon_0 A} \end{equation}\] The electric field is proportional to the surface charge density on either plate of the capacitor.
Example application
A charged particle between two oppositely charged parallel plates undergoes constant acceleration, and therefore its motion shares characteristics with the projectile motion of an object with mass in the gravitational field near the Earth’s surface.
Energy stored in a capacitor
The electric potential energy stored in a capacitor is equal to the work done by an external force to separate that amount of charge on the capacitor. The electric potential energy (\(U_C\)) stored in a capacitor is described by the equation \[\begin{equation} U_C = \dfrac{1}{2} Q \Delta V \end{equation}\] where \(Q\) is the charge and \(\Delta V\) the voltage. Since \(Q=C \Delta V\), this is often also expressed as \[\begin{equation} U_C = \dfrac{1}{2} C V^2 \end{equation}\] especially in the context of electrical engineering.
See also
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