at normal temperature and normal pressure what is the value of permittivity?
Answers
Answer:
In electromagnetism, the absolute permittivity, often simply called permittivity and denoted by the Greek letter ε (epsilon), is a measure of the electric polarizability of a dielectric. A material with high permittivity polarizes more in response to an applied electric field than a material with low permittivity, thereby storing more energy in the electric field. In electrostatics, the permittivity plays an important role in determining the capacitance of a capacitor.
In the simplest case, the electric displacement field {\displaystyle \mathbf {D} }\mathbf{D} resulting from an applied electric field {\displaystyle \mathbf {E} }\mathbf {E} is
{\displaystyle \mathbf {D} =\varepsilon \mathbf {E} .}{\displaystyle \mathbf {D} =\varepsilon \mathbf {E} .}
More generally, the permittivity is a thermodynamic function of state [1]. It can depend on the frequency, magnitude, and direction of the applied field. The SI unit for permittivity is farad per meter (F/m).
The permittivity is often represented by the relative permittivity {\displaystyle \varepsilon _{\textrm {r}}}{\displaystyle \varepsilon _{\textrm {r}}} which is the ratio of the absolute permittivity {\displaystyle \varepsilon }\varepsilon and the vacuum permittivity {\displaystyle \varepsilon _{0}}\varepsilon _{0}
{\displaystyle \kappa =\varepsilon _{r}={\frac {\varepsilon }{\varepsilon _{0}}}}{\displaystyle \kappa =\varepsilon _{r}={\frac {\varepsilon }{\varepsilon _{0}}}}.
This dimensionless quantity is also often and ambiguously referred to as the permittivity. Another common term encountered for both absolute and relative permittivity is the dielectric constant which has been deprecated in physics and engineering[2] as well as in chemistry.[3]
By definition, a perfect vacuum has a relative permittivity of exactly 1 whereas at STP, air has a relative permittivity of κair = 1.0006.
Relative permittivity is directly related to electric susceptibility (χ) by
{\displaystyle \chi =\kappa -1}{\displaystyle \chi =\kappa -1}
otherwise written as
{\displaystyle \varepsilon =\varepsilon _{\mathrm {r} }\varepsilon _{0}=(1+\chi )\varepsilon _{0}}{\displaystyle \varepsilon =\varepsilon _{\mathrm {r} }\varepsilon _{0}=(1+\chi )\varepsilon _{0}}
Explanation: