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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.

- Units
- Explanation
- Vacuum permittivity
- Relative permittivity
- Practical applications
- Determining capacitance
- Gauss's law
- Dispersion and causality
- Complex permittivity
- Tensorial permittivity
- Classification of materials
- Lossy medium
- Quantum-mechanical interpretation
- Measurement
- See also
- Notes
- References
- Further reading
- External links

In the simplest case, the electric displacement field resulting from an applied electric field is

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 which is the ratio of the absolute permittivity and the vacuum permittivity

.

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 *κ*_{air} = 1.0006.

Relative permittivity is directly related to electric susceptibility (*χ*) by

otherwise written as

The standard SI unit for permittivity is farad per meter (F/m or F·m^{−1}).^{ [4] }

In electromagnetism, the electric displacement field **D** represents how an electric field **E** influences the organization of electric charges in a given medium, including charge migration and electric dipole reorientation. Its relation to permittivity in the very simple case of *linear, homogeneous, isotropic * materials with *"instantaneous" response* to changes in electric field is

where the permittivity ε is a scalar. If the medium is anisotropic, the permittivity is a second rank tensor.

In general, permittivity is not a constant, as it can vary with the position in the medium, the frequency of the field applied, humidity, temperature, and other parameters. In a nonlinear medium, the permittivity can depend on the strength of the electric field. Permittivity as a function of frequency can take on real or complex values.

In SI units, permittivity is measured in farads per meter (F/m or A^{2}·s^{4}·kg^{−1}·m^{−3}). The displacement field **D** is measured in units of coulombs per square meter (C/m^{2}), while the electric field **E** is measured in volts per meter (V/m). **D** and **E** describe the interaction between charged objects. **D** is related to the *charge densities* associated with this interaction, while **E** is related to the *forces* and *potential differences*.

The vacuum permittivity *ε*_{0} (also called **permittivity of free space** or the **electric constant**) is the ratio **D**/**E** in free space. It also appears in the Coulomb force constant,

Its value is^{ [5] }

where

*c*_{0}is the speed of light in free space,^{ [lower-alpha 1] }*µ*_{0}is the vacuum permeability.

The constants *c*_{0} and *μ*_{0} were defined in SI units to have exact numerical values until redefinition of SI units in 2019.^{ [7] } (The approximation in the second value of *ε*_{0} above stems from π being an irrational number.)

The linear permittivity of a homogeneous material is usually given relative to that of free space, as a relative permittivity *ε*_{r} (also called dielectric constant, although this term is deprecated and sometimes only refers to the static, zero-frequency relative permittivity). In an anisotropic material, the relative permittivity may be a tensor, causing birefringence. The actual permittivity is then calculated by multiplying the relative permittivity by *ε*_{0}:

where χ (frequently written *χ*_{e}) is the electric susceptibility of the material.

The susceptibility is defined as the constant of proportionality (which may be a tensor) relating an electric field **E** to the induced dielectric polarization density **P** such that

where *ε*_{0} is the electric permittivity of free space.

The susceptibility of a medium is related to its relative permittivity *ε*_{r} by

So in the case of a vacuum,

The susceptibility is also related to the polarizability of individual particles in the medium by the Clausius-Mossotti relation.

The electric displacement **D** is related to the polarization density **P** by

The permittivity ε and permeability µ of a medium together determine the phase velocity *v* = *c*/*n* of electromagnetic radiation through that medium:

The capacitance of a capacitor is based on its design and architecture, meaning it will not change with charging and discharging. The formula for capacitance is written as

where is the area of one plate, is the distance between the plates, and is the permittivity of the medium between the two plates. For a capacitor with relative permittivity , it can be said that

Permittivity is connected to electric flux (and by extension electric field) through Gauss's law. Gauss's law states that for a closed Gaussian surface, s

where is the net electric flux passing through the surface, is the charge enclosed in the Gaussian surface, is the electric field vector at a given point on the surface, and is a differential area vector on the Gaussian surface.

If the Gaussian surface uniformly encloses an insulated, symmetrical charge arrangement, the formula can be simplified to

where represents the angle between the electric field vector and the area vector.

If all of the electric field lines cross the surface at 90°, the formula can be further simplified to

Because the surface area of a sphere is , the electric field a distance away from a uniform, spherical charge arrangement is

where is Coulomb's constant (). This formula applies to the electric field due to a point charge, outside of a conducting sphere or shell, outside of a uniformly charged insulating sphere, or between the plates of a spherical capacitor.

In general, a material cannot polarize instantaneously in response to an applied field, and so the more general formulation as a function of time is

That is, the polarization is a convolution of the electric field at previous times with time-dependent susceptibility given by *χ*(Δ*t*). The upper limit of this integral can be extended to infinity as well if one defines *χ*(Δ*t*) = 0 for Δ*t* < 0. An instantaneous response would correspond to a Dirac delta function susceptibility *χ*(Δ*t*) = *χδ*(Δ*t*).

It is convenient to take the Fourier transform with respect to time and write this relationship as a function of frequency. Because of the convolution theorem, the integral becomes a simple product,

This frequency dependence of the susceptibility leads to frequency dependence of the permittivity. The shape of the susceptibility with respect to frequency characterizes the dispersion properties of the material.

Moreover, the fact that the polarization can only depend on the electric field at previous times (i.e. effectively *χ*(Δ*t*) = 0 for Δ*t* < 0), a consequence of causality, imposes Kramers–Kronig constraints on the susceptibility *χ*(0).

As opposed to the response of a vacuum, the response of normal materials to external fields generally depends on the frequency of the field. This frequency dependence reflects the fact that a material's polarization does not change instantaneously when an electric field is applied. The response must always be *causal* (arising after the applied field), which can be represented by a phase difference. For this reason, permittivity is often treated as a complex function of the (angular) frequency ω of the applied field:

(since complex numbers allow specification of magnitude and phase). The definition of permittivity therefore becomes

where

*D*_{0}and*E*_{0}are the amplitudes of the displacement and electric fields, respectively,- i is the imaginary unit,
*i*^{2}= −1.

The response of a medium to static electric fields is described by the low-frequency limit of permittivity, also called the static permittivity *ε*_{s} (also *ε*_{DC}):

At the high-frequency limit (meaning optical frequencies), the complex permittivity is commonly referred to as *ε*_{∞} (or sometimes *ε*_{opt}^{ [9] }). At the plasma frequency and below, dielectrics behave as ideal metals, with electron gas behavior. The static permittivity is a good approximation for alternating fields of low frequencies, and as the frequency increases a measurable phase difference δ emerges between **D** and **E**. The frequency at which the phase shift becomes noticeable depends on temperature and the details of the medium. For moderate field strength (*E*_{0}), **D** and **E** remain proportional, and

Since the response of materials to alternating fields is characterized by a complex permittivity, it is natural to separate its real and imaginary parts, which is done by convention in the following way:

where

*ε*′ is the real part of the permittivity;*ε*″ is the imaginary part of the permittivity;- δ is the loss angle.

The choice of sign for time-dependence, *e*^{−iωt}, dictates the sign convention for the imaginary part of permittivity. The signs used here correspond to those commonly used in physics, whereas for the engineering convention one should reverse all imaginary quantities.

The complex permittivity is usually a complicated function of frequency ω, since it is a superimposed description of dispersion phenomena occurring at multiple frequencies. The dielectric function *ε*(*ω*) must have poles only for frequencies with positive imaginary parts, and therefore satisfies the Kramers–Kronig relations. However, in the narrow frequency ranges that are often studied in practice, the permittivity can be approximated as frequency-independent or by model functions.

At a given frequency, the imaginary part, *ε*″, leads to absorption loss if it is positive (in the above sign convention) and gain if it is negative. More generally, the imaginary parts of the eigenvalues of the anisotropic dielectric tensor should be considered.

In the case of solids, the complex dielectric function is intimately connected to band structure. The primary quantity that characterizes the electronic structure of any crystalline material is the probability of photon absorption, which is directly related to the imaginary part of the optical dielectric function *ε*(*ω*). The optical dielectric function is given by the fundamental expression:^{ [10] }

In this expression, *W*_{c,v}(*E*) represents the product of the Brillouin zone-averaged transition probability at the energy E with the joint density of states,^{ [11] }^{ [12] }*J*_{c,v}(*E*); φ is a broadening function, representing the role of scattering in smearing out the energy levels.^{ [13] } In general, the broadening is intermediate between Lorentzian and Gaussian;^{ [14] }^{ [15] } for an alloy it is somewhat closer to Gaussian because of strong scattering from statistical fluctuations in the local composition on a nanometer scale.

According to the Drude model of magnetized plasma, a more general expression which takes into account the interaction of the carriers with an alternating electric field at millimeter and microwave frequencies in an axially magnetized semiconductor requires the expression of the permittivity as a non-diagonal tensor.^{ [16] } (see also Electro-gyration).

If *ε*_{2} vanishes, then the tensor is diagonal but not proportional to the identity and the medium is said to be a uniaxial medium, which has similar properties to a uniaxial crystal.

ε_{r}″ / ε_{r}′ | Current conduction | Field propagation |
---|---|---|

0 | perfect dielectric lossless medium | |

≪ 1 | low-conductivity material poor conductor | low-loss medium good dielectric |

≈ 1 | lossy conducting material | lossy propagation medium |

≫ 1 | high-conductivity material good conductor | high-loss medium poor dielectric |

∞ | perfect conductor |

Materials can be classified according to their complex-valued permittivity ε, upon comparison of its real *ε*′ and imaginary *ε*″ components (or, equivalently, conductivity, σ, when accounted for in the latter). A * perfect conductor * has infinite conductivity, *σ* = ∞, while a * perfect dielectric * is a material that has no conductivity at all, *σ* = 0; this latter case, of real-valued permittivity (or complex-valued permittivity with zero imaginary component) is also associated with the name *lossless media*.^{ [17] } Generally, when *σ*/*ωε*′ ≪ 1 we consider the material to be a *low-loss dielectric* (although not exactly lossless), whereas *σ*/*ωε*′ ≫ 1 is associated with a *good conductor*; such materials with non-negligible conductivity yield a large amount of loss that inhibit the propagation of electromagnetic waves, thus are also said to be *lossy media*. Those materials that do not fall under either limit are considered to be general media.

In the case of a lossy medium, i.e. when the conduction current is not negligible, the total current density flowing is:

where

- σ is the conductivity of the medium;
*ε*′ is the real part of the permittivity.- ε̂ is the complex permittivity

The size of the displacement current is dependent on the frequency ω of the applied field *E*; there is no displacement current in a constant field.

In this formalism, the complex permittivity is defined as:^{ [18] }^{ [19] }

In general, the absorption of electromagnetic energy by dielectrics is covered by a few different mechanisms that influence the shape of the permittivity as a function of frequency:

- First are the relaxation effects associated with permanent and induced molecular dipoles. At low frequencies the field changes slowly enough to allow dipoles to reach equilibrium before the field has measurably changed. For frequencies at which dipole orientations cannot follow the applied field because of the viscosity of the medium, absorption of the field's energy leads to energy dissipation. The mechanism of dipoles relaxing is called dielectric relaxation and for ideal dipoles is described by classic Debye relaxation.
- Second are the resonance effects, which arise from the rotations or vibrations of atoms, ions, or electrons. These processes are observed in the neighborhood of their characteristic absorption frequencies.

The above effects often combine to cause non-linear effects within capacitors. For example, dielectric absorption refers to the inability of a capacitor that has been charged for a long time to completely discharge when briefly discharged. Although an ideal capacitor would remain at zero volts after being discharged, real capacitors will develop a small voltage, a phenomenon that is also called *soakage* or *battery action*. For some dielectrics, such as many polymer films, the resulting voltage may be less than 1–2% of the original voltage. However, it can be as much as 15–25% in the case of electrolytic capacitors or supercapacitors.

In terms of quantum mechanics, permittivity is explained by atomic and molecular interactions.

At low frequencies, molecules in polar dielectrics are polarized by an applied electric field, which induces periodic rotations. For example, at the microwave frequency, the microwave field causes the periodic rotation of water molecules, sufficient to break hydrogen bonds. The field does work against the bonds and the energy is absorbed by the material as heat. This is why microwave ovens work very well for materials containing water. There are two maxima of the imaginary component (the absorptive index) of water, one at the microwave frequency, and the other at far ultraviolet (UV) frequency. Both of these resonances are at higher frequencies than the operating frequency of microwave ovens.

At moderate frequencies, the energy is too high to cause rotation, yet too low to affect electrons directly, and is absorbed in the form of resonant molecular vibrations. In water, this is where the absorptive index starts to drop sharply, and the minimum of the imaginary permittivity is at the frequency of blue light (optical regime).

At high frequencies (such as UV and above), molecules cannot relax, and the energy is purely absorbed by atoms, exciting electron energy levels. Thus, these frequencies are classified as ionizing radiation.

While carrying out a complete * ab initio * (that is, first-principles) modelling is now computationally possible, it has not been widely applied yet. Thus, a phenomenological model is accepted as being an adequate method of capturing experimental behaviors. The Debye model and the Lorentz model use a first-order and second-order (respectively) lumped system parameter linear representation (such as an RC and an LRC resonant circuit).

The relative permittivity of a material can be found by a variety of static electrical measurements. The complex permittivity is evaluated over a wide range of frequencies by using different variants of dielectric spectroscopy, covering nearly 21 orders of magnitude from 10^{−6} to 10^{15} hertz. Also, by using cryostats and ovens, the dielectric properties of a medium can be characterized over an array of temperatures. In order to study systems for such diverse excitation fields, a number of measurement setups are used, each adequate for a special frequency range.

Various microwave measurement techniques are outlined in Chen *et al.*.^{ [20] } Typical errors for the Hakki-Coleman method employing a puck of material between conducting planes are about 0.3%.^{ [21] }

- Low-frequency time domain measurements (10
^{−6}to 10^{3}Hz) - Low-frequency frequency domain measurements (10
^{−5}to 10^{6}Hz) - Reflective coaxial methods (10
^{6}to 10^{10}Hz) - Transmission coaxial method (10
^{8}to 10^{11}Hz) - Quasi-optical methods (10
^{9}to 10^{10}Hz) - Terahertz time-domain spectroscopy (10
^{11}to 10^{13}Hz) - Fourier-transform methods (10
^{11}to 10^{15}Hz)

At infrared and optical frequencies, a common technique is ellipsometry. Dual polarisation interferometry is also used to measure the complex refractive index for very thin films at optical frequencies.

**Nonlinear optics** (**NLO**) is the branch of optics that describes the behaviour of light in *nonlinear media*, that is, media in which the polarization density **P** responds non-linearly to the electric field **E** of the light. The non-linearity is typically observed only at very high light intensities (values of atomic electric fields, typically 10^{8} V/m) such as those provided by lasers. Above the Schwinger limit, the vacuum itself is expected to become nonlinear. In nonlinear optics, the superposition principle no longer holds.

A **dielectric** is an electrical insulator that can be polarized by an applied electric field. When a dielectric is placed in an electric field, electric charges do not flow through the material as they do in an electrical conductor but only slightly shift from their average equilibrium positions causing **dielectric polarization**. Because of dielectric polarization, positive charges are displaced in the direction of the field and negative charges shift in the direction opposite to the field. This creates an internal electric field that reduces the overall field within the dielectric itself. If a dielectric is composed of weakly bonded molecules, those molecules not only become polarized, but also reorient so that their symmetry axes align to the field.

The **wave impedance** of an electromagnetic wave is the ratio of the transverse components of the electric and magnetic fields. For a transverse-electric-magnetic (TEM) plane wave traveling through a homogeneous medium, the wave impedance is everywhere equal to the intrinsic impedance of the medium. In particular, for a plane wave travelling through empty space, the wave impedance is equal to the impedance of free space. The symbol *Z* is used to represent it and it is expressed in units of ohms. The symbol *η* (eta) may be used instead of *Z* for wave impedance to avoid confusion with electrical impedance.

In physics, the **Poynting vector** represents the directional energy flux of an electromagnetic field. The SI unit of the Poynting vector is the watt per square metre (W/m^{2}). It is named after its discoverer John Henry Poynting who first derived it in 1884. Oliver Heaviside also discovered it independently.

The **relative permittivity** of a material is its (absolute) permittivity expressed as a ratio relative to the vacuum permittivity.

In physics, **Gauss's law**, also known as **Gauss's flux theorem**, is a law relating the distribution of electric charge to the resulting electric field. The surface under consideration may be a closed one enclosing a volume such as a spherical surface.

**Crystal optics** is the branch of optics that describes the behaviour of light in *anisotropic media*, that is, media in which light behaves differently depending on which direction the light is propagating. The index of refraction depends on both composition and crystal structure and can be calculated using the Gladstone–Dale relation. Crystals are often naturally anisotropic, and in some media it is possible to induce anisotropy by applying an external electric field.

In physics, **screening** is the damping of electric fields caused by the presence of mobile charge carriers. It is an important part of the behavior of charge-carrying fluids, such as ionized gases, electrolytes, and charge carriers in electronic conductors . In a fluid, with a given permittivity *ε*, composed of electrically charged constituent particles, each pair of particles interact through the Coulomb force as

In physics, the **dissipation factor** (DF) is a measure of loss-rate of energy of a mode of oscillation in a dissipative system. It is the reciprocal of quality factor, which represents the "quality" or durability of oscillation.

The **Kerr effect**, also called the **quadratic electro-optic** (**QEO**) **effect**, is a change in the refractive index of a material in response to an applied electric field. The Kerr effect is distinct from the Pockels effect in that the induced index change is directly proportional to the *square* of the electric field instead of varying linearly with it. All materials show a Kerr effect, but certain liquids display it more strongly than others. The Kerr effect was discovered in 1875 by John Kerr, a Scottish physicist.

In classical electromagnetism, **polarization density** is the vector field that expresses the density of permanent or induced electric dipole moments in a dielectric material. When a dielectric is placed in an external electric field, its molecules gain electric dipole moment and the dielectric is said to be polarized. The electric dipole moment induced per unit volume of the dielectric material is called the electric polarization of the dielectric.

In electricity (electromagnetism), the **electric susceptibility** is a dimensionless proportionality constant that indicates the degree of polarization of a dielectric material in response to an applied electric field. The greater the electric susceptibility, the greater the ability of a material to polarize in response to the field, and thereby reduce the total electric field inside the material. It is in this way that the electric susceptibility influences the electric permittivity of the material and thus influences many other phenomena in that medium, from the capacitance of capacitors to the speed of light.

In physics, the **electric displacement field**, denoted by **D**, is a vector field that appears in Maxwell's equations. It accounts for the effects of free and bound charge within materials. "**D**" stands for "displacement", as in the related concept of displacement current in dielectrics. In free space, the electric displacement field is equivalent to flux density, a concept that lends understanding to Gauss's law. In the International System of Units (SI), it is expressed in units of coulomb per meter square (C⋅m^{−2}).

A **capacitor** is a device that stores electrical energy in an electric field. It is a passive electronic component with two terminals.

**Dielectric loss** quantifies a dielectric material's inherent dissipation of electromagnetic energy. It can be parameterized in terms of either the **loss angle***δ* or the corresponding **loss tangent** tan *δ*. Both refer to the phasor in the complex plane whose real and imaginary parts are the resistive (lossy) component of an electromagnetic field and its reactive (lossless) counterpart.

When an electromagnetic wave travels through a medium in which it gets attenuated, it undergoes exponential decay as described by the Beer–Lambert law. However, there are many possible ways to characterize the wave and how quickly it is attenuated. This article describes the mathematical relationships among:

The **optical conductivity** is a material property, which links the current density to the electric field for general frequencies. In this sense, this linear response function is a generalization of the electrical conductivity, which is usually considered in the static limit, i.e., for a time-independent electric field. While the static electrical conductivity is vanishingly small in insulators, the optical conductivity always remains finite in some frequency intervals ; the total **optical weight** can be inferred from sum rules. The optical conductivity is closely related to the dielectric function, the generalization of the dielectric constant to arbitrary frequencies.

**Surface plasmon polaritons** (**SPPs**) are electromagnetic waves that travel along a metal–dielectric or metal–air interface, practically in the infrared or visible-frequency. The term "surface plasmon polariton" explains that the wave involves both charge motion in the metal and electromagnetic waves in the air or dielectric ("polariton").

In optics, **Miller's rule** is an empirical rule which gives an estimate of the order of magnitude of the nonlinear coefficient.

In optics, the **Ewald–Oseen extinction theorem**, sometimes referred to as just "extinction theorem", is a theorem that underlies the common understanding of scattering. It is named after Paul Peter Ewald and Carl Wilhelm Oseen, who proved the theorem in crystalline and isotropic media, respectively, in 1916 and 1915. Originally, the theorem applied to scattering by an isotropic dielectric objects in free space. The scope of the theorem was greatly extended to encompass a wide variety of bianisotropic media.

- ↑ Landau, L. D.; Lifshitz, E. M.; Pitaevskii, L. P. (2009).
*Electrodynamics of continuous media*. Elsevier Butterworth-Heinemann. ISBN 978-0-7506-2634-7. OCLC 756385298. - ↑ IEEE Standards Board (1997). "IEEE Standard Definitions of Terms for Radio Wave Propagation". p. 6.
- ↑ Braslavsky, S.E. (2007). "Glossary of terms used in photochemistry (IUPAC recommendations 2006)" (PDF).
*Pure and Applied Chemistry*.**79**(3): 293–465. doi:10.1351/pac200779030293. - ↑ International Bureau of Weights and Measures (2006),
*The International System of Units (SI)*(PDF) (8th ed.), ISBN 92-822-2213-6, archived (PDF) from the original on 2017-08-14, p. 119 - ↑ "2018 CODATA Value: vacuum electric permittivity".
*The NIST Reference on Constants, Units, and Uncertainty*. NIST. 20 May 2019. Retrieved 2019-05-20. - ↑ NIST
*Special Publication 330*, Appendix 2, p. 45 . - ↑ "Latest (2006) values of the constants (NIST)". Physics.nist.gov. 2017-07-01. Retrieved 2018-11-20.
- ↑ "Dielectric Spectroscopy" . Retrieved 2018-11-20.
- ↑ Hofmann, Philip (2015-05-26).
*Solid State Physics*(2 ed.). Wiley-VCH. p. 194. ISBN 978-3527412822. - ↑ Peter Y. Yu; Manuel Cardona (2001).
*Fundamentals of Semiconductors: Physics and Materials Properties*. Berlin: Springer. p. 261. ISBN 978-3-540-25470-6. - ↑ José García Solé, Jose Solé, Luisa Bausa (2001).
*An introduction to the optical spectroscopy of inorganic solids*. Wiley. Appendix A1, pp, 263. ISBN 978-0-470-86885-0.CS1 maint: multiple names: authors list (link) - ↑ John H. Moore; Nicholas D. Spencer (2001).
*Encyclopedia of chemical physics and physical chemistry*. Taylor and Francis. p. 105. ISBN 978-0-7503-0798-7. - ↑ Solé, José García; Bausá, Louisa E; Jaque, Daniel (2005-03-22).
*Solé and Bausa*. p. 10. ISBN 978-3-540-25470-6. - ↑ Hartmut Haug; Stephan W. Koch (1994).
*Quantum Theory of the Optical and Electronic Properties of Semiconductors*. World Scientific. p. 196. ISBN 978-981-02-1864-5. - ↑ Manijeh Razeghi (2006).
*Fundamentals of Solid State Engineering*. Birkhauser. p. 383. ISBN 978-0-387-28152-0. - ↑ Prati E. (2003) "Propagation in gyroelectromagnetic guiding systems",
*J. of Electr. Wav. and Appl.***17, 8**, 1177 - ↑ http://www.ece.rutgers.edu/~orfanidi/ewa/ch01.pdf
- ↑ John S. Seybold (2005),
*Introduction to RF Propagation*, John Wiley & Sons, p. 22, eq. (2.6). - ↑ Kenneth L. Kaiser,
*Electromagnetic Shielding*, CRC Press, 2005, p. 1·28, eqs. (1.80) and (1.81). - ↑ Linfeng Chen; V. V. Varadan; C. K. Ong; Chye Poh Neo (2004). "Microwave theory and techniques for materials characterization".
*Microwave electronics*. Wiley. p. 37. ISBN 978-0-470-84492-2. - ↑ Mailadil T. Sebastian (2008).
*Dielectric Materials for Wireless Communication*. Elsevier. p. 19. ISBN 978-0-08-045330-9.

- C. J. F. Bottcher, O. C. von Belle & Paul Bordewijk (1973)
*Theory of Electric Polarization: Dielectric Polarization*, volume 1, (1978) volume 2, Elsevier ISBN 0-444-41579-3. - Arthur R. von Hippel (1954)
*Dielectrics and Waves*ISBN 0-89006-803-8 - Arthur von Hippel editor (1966)
*Dielectric Materials and Applications: papers by 22 contributors*ISBN 0-89006-805-4.

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