Relative permittivity

In physics, in particular in electrostatics, the relative permittivity (also known by the now obsolescent term dielectric constant) is an intrinsic property of a non-conducting material, a dielectric. It is usually denoted by ε_r and is the proportionality constant between the electric field and the electric displacement. The relative permittivity describes the ease by which a dielectric medium may be polarized. The capacitance of a capacitor is proportional to ε_r.

When two electric charges are placed inside a dielectric, the electrostatic force between the charges is changed by a factor 1/ε_r. Empirically it is observed that the force between two charges never increases (the force stays the same or decreases) by the presence of any dielectric medium, hence the relative permittivity ε_r ≥ 1. Only the vacuum has ε_r = 1 (exact); all dielectrics have values larger than one (but some materials, such as non-dense inert gases, have relative permittivities very close to the vacuum value of unity).

Definition by capacitance of parallel-plate capacitor

An common alternative definition invokes parallel-plate capacitors. In order to make the connection, it must be first pointed out that it follows from Coulomb's law that the electric field above a charged plate of infinite size is independent of the distance from the plate. (This will be shown in the next section.) If σ is the charge density on the plate (charge per surface, in SI units C/m²), it will be shown that the strength E of the field E is given by

E = σ/(2 ε₀ε_r),

where ε₀ is the electric constant. In Gaussian units one may take ε₀ = 1. When the charge density σ is positive the electric field (a vector) E points away from the plate. Of course, plates of infinite size do not exist, but this formula is applicable when the height is much smaller than the dimensions of the plate, so that border effects can be neglected.

In parallel-plate capacitors border effects can usually be ignored and because both plates have the same charge density (but of opposite sign), the electric field inside a capacitor, filled with a dielectric with ε_r, is double that of one plate

E = σ/(ε₀ε_r).

If the plates have surface area A, they carry a total charge Q = σ A (positive on one plate, negative on the other),

Q = ε₀ε_r A E.

Say the distance between the plates is d, then the voltage difference V between the plates is E / d.

The capacitance C of a capacitor is by definition Q / V, so that we find that the capacitance of a parallel-plate capacitor is linear in the relative permittivity ε_r:

C = ε_r C₀ with C₀ ≡ ε₀ A / d.

Clearly, C₀ is the capacity with vacuum between the plates, and

ε_r = C/C₀.

This property of capacitors is often used as the definition of relative permittivity: ε_r is equal to the ratio of the capacitance of a capacitor filled with the dielectric to the capacitance of an identical capacitor in a vacuum without the dielectric material.

Because ε_r > 1, the insertion of a dielectric between the plates of a parallel-plate capacitor always increases its capacitance, or ability to store opposite charges on each plate, compared with this ability when the plates are separated by a vacuum.

The relative permittivity is defined as a macroscopic property of dielectrics, without need of specifying the electrical behavior of the material on the atomic scale.

Electric field above infinite plate

To compute E we let the charged plate be in the x-y plane. It is a priori clear from the symmetry of the problem that the field at a point z on the z-axis has only a z component, the field components parallel to the plate are always compensated by corresponding negative components.

Use that an infinitesimal surface element in cylinder coordinates times the surface charge density σ gives an infinitesimal charge in the plate,

$\mathrm {d} Q=\sigma \;r\;\mathrm {d} r\mathrm {d} \varphi \,,$

where σ is assumed constant over the plate and for convenience sake we take it positive (hence the field points in the positive z direction). The electric field in the z direction at a point (0,0,z) is by Coulomb's law

$\mathrm {d} E_{z}={\frac {R_{z}\mathrm {d} Q}{4\pi \epsilon _{0}\epsilon _{r}R^{3}}}={\frac {\sigma zr\mathrm {d} r\mathrm {d} \varphi }{4\pi \epsilon _{0}\epsilon _{r}(r^{2}+z^{2})^{3/2}}}.$

Integration over φ gives a factor 2π and

$E_{z}={\frac {z\sigma }{2\epsilon _{0}\epsilon _{r}}}\int _{0}^{\infty }{\frac {r}{(r^{2}+z^{2})^{3/2}}}\;\mathrm {d} r={\frac {\sigma }{2\epsilon _{0}\epsilon _{r}}}.$

Often one defines the electric displacement by D ≡ ε₀ε_rE. Cleary D_z depends only on the charge density and not on the permittivity,

$D_{z}={\frac {1}{2}}\sigma .$

The fact that E and D do not depend on the distance of the field point to the plate may be compared with the gravitational force, −mg, being independent of height close to the surface of the Earth.