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What is "the conductivity we usually use"use”? 

You apply an electric field E$E$ to a solid and get a current j=\sigma E$j = \sigma E$. The proportionality coefficient \sigma$\sigma$ is the conductivity. 

If you apply a time-independent electric field, the conductivity \sigma$\sigma$ is a just a number and is the static conductivity of the medium. If you apply a time-dependent electric field, e.g. E(t)=E_0\cos(\omega t)$E \left( t \right) = E_{0} \cos \left( \omega t \right)$, the conductivity \sigma(\omega)$\sigma \left( \omega \right)$ becomes a function of the frequency \omega$\omega$ and is the dynamic conductivity of the medium. 

The static conductivity \sigma(\omega=0)$\sigma \left( \omega = 0 \right)$ is a special case of the dynamic conductivity. The static conductivity of a dielectric is zero. The dynamic conductivity of any medium, including dielectrics, is always finite. The

The sentence "ac conductivity might be considered a form of impedance spectroscopy" in the previous answer ifis meaningless, since the conductivity is a physical quantity which characterizes a medium, while any spectroscopy is an experimental method to measure some physical properties of a medium, e.g. the dynamic conductivity.

What is "the conductivity we usually use"? You apply an electric field E to a solid and get a current j=\sigma E. The proportionality coefficient \sigma is the conductivity. If you apply a time-independent electric field, the conductivity \sigma is a just a number and is the static conductivity of the medium. If you apply a time-dependent electric field, e.g. E(t)=E_0\cos(\omega t), the conductivity \sigma(\omega) becomes a function of the frequency \omega and is the dynamic conductivity of the medium. The static conductivity \sigma(\omega=0) is a special case of the dynamic conductivity. The static conductivity of a dielectric is zero. The dynamic conductivity of any medium, including dielectrics, is always finite. The sentence "ac conductivity might be considered a form of impedance spectroscopy" in the previous answer if meaningless, since the conductivity is a physical quantity which characterizes a medium, while any spectroscopy is an experimental method to measure some physical properties of a medium, e.g. the dynamic conductivity.

What is "the conductivity we usually use”? 

You apply an electric field $E$ to a solid and get a current $j = \sigma E$. The proportionality coefficient $\sigma$ is the conductivity. 

If you apply a time-independent electric field, the conductivity $\sigma$ is just a number and is the static conductivity of the medium. If you apply a time-dependent electric field, e.g. $E \left( t \right) = E_{0} \cos \left( \omega t \right)$, the conductivity $\sigma \left( \omega \right)$ becomes a function of the frequency $\omega$ and is the dynamic conductivity of the medium. 

The static conductivity $\sigma \left( \omega = 0 \right)$ is a special case of the dynamic conductivity. The static conductivity of a dielectric is zero. The dynamic conductivity of any medium, including dielectrics, is always finite.

The sentence "ac conductivity might be considered a form of impedance spectroscopy" in the previous answer is meaningless, since conductivity is a physical quantity which characterizes a medium, while any spectroscopy is an experimental method to measure some physical properties of a medium, e.g. the dynamic conductivity.

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What is "the conductivity we usually use"? You apply an electric field E to a solid and get a current j=\sigma E. The proportionality coefficient \sigma is the conductivity. If you apply a time-independent electric field, the conductivity \sigma is a just a number and is the static conductivity of the medium. If you apply a time-dependent electric field, e.g. E(t)=E_0\cos(\omega t), the conductivity \sigma(\omega) becomes a function of the frequency \omega and is the dynamic conductivity of the medium. The static conductivity \sigma(\omega=0) is a special case of the dynamic conductivity. The static conductivity of a dielectric is zero. The dynamic conductivity of any medium, including dielectrics, is always finite. The sentence "ac conductivity might be considered a form of impedance spectroscopy" in the previous answer if meaningless, since the conductivity is a physical quantity which characterizes a medium, while any spectroscopy is an experimental method to measure some physical properties of a medium, e.g. the dynamic conductivity.