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In [[electromagnetism]], the '''electric susceptibility''' <math>\chi_{\text{e}}</math> ([[latin]]: ''susceptibilis'' “receptive”) is a dimensionless proportionality constant that indicates the degree of [[polarization (electrostatics)|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 (and store energy). 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]].<ref name=brit>
{{Cite encyclopedia
  | title =Electric susceptibility
  | encyclopedia =[[Encyclopædia Britannica]]
}}</ref><ref name=Cardarelli>
{{Cite book
  | last = Cardarelli
  | first =François
  | title =Materials Handbook: A Concise Desktop Reference
  | publisher =[[Springer-Verlag]]
  | edition =2nd
  | date =2000, 2008
  | location =London
  | pages =524 (Section 8.1.16)
  | url =http://books.google.com/books?id=PvU-qbQJq7IC&pg=PA524&dq=Electric+susceptibility#v=onepage&q=Electric%20susceptibility&f=false
  | doi =10.1007/978-1-84628-669-8
  | isbn =978-1-84628-668-1
  | mr =
  | zbl =
  | jfm = }}</ref>
 
==Definition of volume susceptibility==
 
Electric susceptibility is defined as the constant of proportionality (which may be a [[tensor]]) relating an [[electric field]] '''E''' to the induced [[dielectric]] [[polarization (electrostatics)|polarization density]] '''P''' such that:
 
:<math>{\mathbf P}=\varepsilon_0\chi_{\text{e}}{\mathbf E},</math>
 
where
* <math>\mathbf{P}</math> is the polarization density;
* <math>\varepsilon_0</math> is the [[Vacuum permittivity|electric permittivity of free space]];
* <math>\chi_{\textrm{e}}</math> is the electric susceptibility;
* <math>\mathbf{E}</math> is the electric field.
 
The susceptibility is also related to the [[polarizability]] of individual particles in the medium by the [[Clausius-Mossotti relation]]. The susceptibility is related to its [[relative permittivity]] <math>\varepsilon_{\textrm{r}}</math> by:
 
:<math>\chi_{\text{e}}\ = \varepsilon_{\text{r}} - 1</math>
 
So in the case of a vacuum:
 
:<math>\chi_{\text{e}}\ =  0</math>
 
At the same time, the [[electric displacement]] '''D''' is related to the polarization density '''P''' by:
 
:<math>\mathbf{D} \ = \ \varepsilon_0\mathbf{E} + \mathbf{P} \ = \ \varepsilon_0 (1+\chi_{\text{e}}) \mathbf{E} \ = \ \varepsilon_{\text{r}} \varepsilon_0 \mathbf{E}.</math>
 
==Molecular polarizability==
 
A similar parameter exists to relate the magnitude of the induced [[Molecular dipole moment|dipole moment]] '''p''' of an individual [[molecule]] to the local electric field '''E''' that induced the dipole. This parameter is the ''molecular polarizability'' and the dipole moment resulting from the local electric field '''E'''<sub>local</sub> is given by:
 
:<math>\mathbf{p}=\varepsilon_0\alpha \mathbf{E_{\text{local}}}</math>
 
This introduces a complication however, as locally the field can differ significantly from the overall applied field. We have:
 
:<math>\mathbf{P} = N \mathbf{p} = N \varepsilon_0 \alpha \mathbf{E}_\text{local},</math>
 
where '''P''' is the polarization per unit volume, and ''N'' is the number of molecules per unit volume contributing to the polarization. Thus, if the local electric field is parallel to the ambient electric field, we have:
 
:<math>\chi_{\text{e}} \mathbf{E} = N \alpha \mathbf{E}_{\text{local}}</math>
 
Thus only if the local field equals the ambient field can we write:
 
:<math>\chi_{\text{e}}\ = N \alpha</math>
 
== Nonlinear susceptibility ==
 
In many materials the polarizability starts to saturate at high values of electric field. This saturation can be modelled by a '''nonlinear susceptibility'''. These susceptibilities are important in [[nonlinear optics]] and lead to effects such as [[second harmonic generation]] (such as used to convert infrared light into visible light, in green [[laser pointer]]s).
 
The standard definition of nonlinear susceptibilities in SI units is via a [[Taylor expansion]] of the polarization's reaction to electric field:<ref>Paul N. Butcher, David Cotter, ''The Elements of Nonlinear Optics''</ref>
:<math> P = P_0 + \varepsilon_0 \chi^{(1)} E + \varepsilon_0 \chi^{(2)} E^2 + \varepsilon_0 \chi^{(3)} E^3 + \cdots. </math>
(Except in [[ferroelectric]] materials, the built-in polarization is zero, <math>P_0 = 0</math>.)
The first susceptibility term, <math>\chi^{(1)}</math>, corresponds to the linear susceptibility described above. While this first term is dimensionless, the subsequent nonlinear susceptibilities <math>\chi^{(n)}</math> have units of {{math|(m/V)<sup>''n''-1</sup>}}.
 
The nonlinear susceptibilities can be generalized to anisotropic materials (where each susceptibility <math>\chi^{(n)}</math> becomes an ''n+1''-rank [[tensor]]).
 
==Dispersion and causality==
 
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
 
:<math>\mathbf{P}(t)=\varepsilon_0 \int_{-\infty}^t \chi_{\text{e}}(t-t') \mathbf{E}(t')\, dt'.</math>
 
That is, the polarization is a [[convolution]] of the electric field at previous times with time-dependent susceptibility given by <math>\chi_{\text{e}}(\Delta t)</math>.   The upper limit of this integral can be extended to infinity as well if one defines <math>\chi_{\text{e}}(\Delta t) = 0</math> for <math>\Delta t < 0</math>. An instantaneous response corresponds to [[Dirac delta function]] susceptibility <math>\chi_{\text{e}}(\Delta t) = \chi_{\text{e}}\delta(\Delta t)</math>.
 
It is more convenient in a linear system to take the [[continuous Fourier transform|Fourier transform]] and write this relationship as a function of frequency. Due to the [[convolution theorem]], the integral becomes a simple product,
 
:<math>\mathbf{P}(\omega) = \varepsilon_0 \chi_{\text{e}}(\omega) \mathbf{E}(\omega).</math>
 
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 (optics)|dispersion]] properties of the material.
 
Moreover, the fact that the polarization can only depend on the electric field at previous times (i.e. <math>\chi_{\text{e}}(\Delta t) = 0</math> for <math>\Delta t < 0</math>), a consequence of [[causality]], imposes [[Kramers–Kronig relation|Kramers–Kronig constraints]] on the susceptibility <math>\chi_{\text{e}}(0)</math>.
 
==See also==
 
* [[Application of tensor theory in physics]]
* [[Magnetic susceptibility]]
* [[Maxwell's equations]]
* [[Permittivity]]
* [[Clausius-Mossotti relation]]
* [[Linear response function]]
* [[Green–Kubo relations]]
 
==References==
{{reflist}}
 
[[Category:Electric and magnetic fields in matter]]
[[Category:Physical quantities]]
 
[[uk:Поляризовність]]

Latest revision as of 06:53, 29 September 2014

Douglass Community also preserves the biggest ceiling servicing miramar office of any service provider in the state of Co. With very few repairs and maintenance jobs required for an in depth period after its installation, EPDM has demonstrated for being the single most inexpensive and protective roofing materials you should purchase. Otherwise, they are deductible on Schedule E (rental) or Schedule A (resale property). In spite of this, many proprietors don't elegance properly. One reason being that we tend to find things to fall over when we do.

' Felt roofs - Because they're specified and installed correctly, our range of traditional and rubber flat roofs will provide you with decades of trouble free service. Magazine articles about this subject show some great alternatives including great colors as well as white housetops which are capable of great heat reflection and energy-saving during hot weather months. Terracotta roof tiles have been superseded by concrete roof tiles. For composition roofs (the most common type), granules, or lack there of, are the primary indicator of remaining roof life, much like the tread on a tire. A chief thing to consider when deciding on roof repair in Portland or an entirely new roof is the age of your existing roof.

Roofers of Las Vegas is a roofing service provider which offers an array of services for both residential and commercial purposes. Portland Oregon contractors who offer competitive pricing will often include a free quote as part of standard protocol. Every year a small amount of the shake surface is worn away by the sun and weather. Metal roofing, experts suggest, will net you the largest premium discount, but comes with a heavier price tag. For a pitched roof generally an asphalt shingle certainly is the cheapest to replace.

A great roof repair tip that can prevent shingles or shakes from pulling up, and that can also prevent mildew or mould, is to cut away all tree limbs that rest against your roof. Carefully come down off the roof and remove the ladder. Eternabond is a repair tape that will work on all surfaces- metal, fiberglass, rubber and vinyl. Metal roofing is one of the more popular options for commercial business roofing applications. If you treasured this article and you would like to obtain more info relating to San Antonio metal roof repair kindly visit our own website. As one of the important aspects of a house, a roof must be well-maintained and repaired from time to time in order for it to function efficiently.

The primary thing that you will need to repair your loose tiles is a tube of roofing cement. You may utilize online resources or seek recommendations from those you know and trust. They must carry both a city business license and a contractor. Going through the printed material is not easy as it will consume a lot of your time and the credibility of the written material may vary too. Make sure you leave enough and proper space and inclination in this marking.