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<j.1:description rdf:datatype="http://qudt.org/schema/qudt/LatexString">The $\textit{relative permittivity}$ of a material under given conditions reflects the extent to which it concentrates electrostatic lines of flux. In technical terms, it is the ratio of the amount of electrical energy stored in a material by an applied voltage, relative to that stored in a vacuum. Likewise, it is also the ratio of the capacitance of a capacitor using that material as a dielectric, compared to a similar capacitor that has a vacuum as its dielectric. Relative permittivity is a dimensionless number that is in general complex. The imaginary portion of the permittivity corresponds to a phase shift of the polarization P relative to E and leads to the attenuation of electromagnetic waves passing through the medium.</p>
<p>$\epsilon_r(w) = \frac{\epsilon(w)}{\epsilon_O}$\ where $\epsilon_r(w)$ is the complex frequency-dependent absolute permittivity of the material, and $\epsilon_O$ is the vacuum permittivity.</j.1:description>
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<p>$\\epsilon_r(w) = \\frac{\\epsilon(w)}{\\epsilon_O}$\\ where $\\epsilon_r(w)$ is the complex frequency-dependent absolute permittivity of the material, and $\\epsilon_O$ is the vacuum permittivity."""^^<http://qudt.org/schema/qudt/LatexString> ;
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