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  2. Perfect conductor - Wikipedia

    en.wikipedia.org/wiki/Perfect_conductor

    In electrostatics, a perfect conductor is an idealized model for real conducting materials. The defining property of a perfect conductor is that static electric field and the charge density both vanish in its interior. If the conductor has excess charge, it accumulates as an infinitesimally thin layer of surface charge. An external electric ...

  3. Interface conditions for electromagnetic fields - Wikipedia

    en.wikipedia.org/wiki/Interface_conditions_for...

    This is done by assuming conditions at the boundaries which are physically correct and numerically solvable in finite time. In some cases, the boundary conditions resume to a simple interface condition. The most usual and simple example is a fully reflecting (electric wall) boundary - the outer medium is considered as a perfect conductor.

  4. Electricity - Wikipedia

    en.wikipedia.org/wiki/Electricity

    Maxwell's equations, which unify light, fields, and charge are one of the great milestones of theoretical physics. [ 25 ] : 696–700 The work of many researchers enabled the use of electronics to convert signals into high frequency oscillating currents and, via suitably shaped conductors, electricity permits the transmission and reception of ...

  5. Perfect mirror - Wikipedia

    en.wikipedia.org/wiki/Perfect_mirror

    A very complex dielectric mirror can reflect up to 99.999% of the light incident upon it, for a narrow range of wavelengths and angles. A simpler mirror may reflect 99.9% of the light, but may cover a broader range of wavelengths. Almost any dielectric material can act as a perfect mirror through total internal reflection. This effect only ...

  6. Talk:Perfect conductor - Wikipedia

    en.wikipedia.org/wiki/Talk:Perfect_conductor

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  7. Characteristic impedance - Wikipedia

    en.wikipedia.org/wiki/Characteristic_impedance

    This would imply that the conductors act like perfect conductors and the dielectric acts like a perfect dielectric. For a lossless line, R and G are both zero, so the equation for characteristic impedance derived above reduces to: =.

  8. London equations - Wikipedia

    en.wikipedia.org/wiki/London_equations

    There are two London equations when expressed in terms of measurable fields: =, =. Here is the (superconducting) current density, E and B are respectively the electric and magnetic fields within the superconductor, is the charge of an electron or proton, is electron mass, and is a phenomenological constant loosely associated with a number density of superconducting carriers.

  9. Extraordinary optical transmission - Wikipedia

    en.wikipedia.org/wiki/Extraordinary_optical...

    Interference pattern of double slits, where the slit width is one third the wavelength. Extraordinary optical transmission (EOT) is the phenomenon of greatly enhanced transmission of light through a subwavelength aperture in an otherwise opaque metallic film which has been patterned with a regularly repeating periodic structure.