Fresnel equations

The Fresnel equations describe the amplitudes of light reflected and transmitted at an interface between optical media. They account for the incident angle, refractive indices and polarization, distinguishing s-polarized light from p-polarized light. From the amplitude coefficients, reflectance and transmittance can be calculated; the equations also explain effects such as the disappearance of p-polarized reflection at Brewster's angle.

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30 October 2026
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What the equations describe

When a light wave reaches a boundary between two media, part of its energy may be reflected and part transmitted. The Fresnel equations give the amplitude reflection and transmission coefficients at a flat interface, under specified optical conditions. Their inputs include the refractive indices of the media and the directions of the incident and transmitted waves; the latter are related by Snell's law. The equations follow from electromagnetic boundary conditions at the interface.

Polarization at an interface

For a ray meeting a surface, the plane of incidence contains the incident ray and the surface normal. In s polarization, the electric field is perpendicular to this plane; in p polarization, it lies within it. The Fresnel equations give distinct coefficients for these two cases, so the amount of reflected light generally depends on polarization as well as angle and material. For unpolarized light, reflectance can be found by combining the two polarization contributions with the appropriate averaging.

From amplitudes to power

The reflection coefficient describes the reflected electric-field amplitude relative to the incident amplitude. For a non-absorbing interface, the reflectance for a given polarization is the squared magnitude of its amplitude reflection coefficient. Converting a transmission amplitude into transmitted power also requires a factor accounting for the refractive indices and propagation angles. At normal incidence between transparent, non-absorbing media, the reflectance is R = ((n₁ − n₂)/(n₁ + n₂))², where n₁ and n₂ are the refractive indices.

Brewster's angle and practical use

For a transparent dielectric boundary, the p-polarized reflection coefficient becomes zero at Brewster's angle. At that angle, reflected unpolarized light is s-polarized. Fresnel calculations are used to estimate reflection losses and design optical systems, including lenses, windows and laser resonators. The basic transparent-medium formulas require care for absorbing materials: these can be treated using a complex refractive index, and transmitted power must be calculated with attention to absorption and energy flow.

Key facts

Purpose
Calculate reflected and transmitted light amplitudes at an optical interface.
Polarization cases
The equations distinguish s polarization (electric field perpendicular to the plane of incidence) and p polarization (electric field within it).
Reflectance
For a given polarization, reflectance is the squared magnitude of the amplitude reflection coefficient.
Brewster's angle
At a transparent dielectric interface, p-polarized reflection vanishes at this angle.
Applications
Optical design uses Fresnel equations to calculate surface reflection and transmission.

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References

  1. 1.
    Fresnel Equations

    University of Arizona, College of Optical Sciences · other · reliability: unverified · retrieved 30 October 2026

    Supports: Explains Fresnel amplitude coefficients, s and p polarization, field continuity at a boundary, and conversion from amplitudes to irradiance quantities.

  2. 2.
    Fresnel Equations

    RP Photonics Encyclopedia · other · reliability: unverified · retrieved 30 October 2026

    Supports: Defines Fresnel coefficients for s and p polarization, describes reflectance and transmittance calculations, normal-incidence reflectivity, Brewster-angle behavior, and the use of complex refractive indices for absorbing media.

  3. 3.
    Fresnel Equations for Polarization

    Ocean Optics Web Book · other · reliability: unverified · retrieved 30 October 2026

    Supports: Discusses reflection and transmission of polarized light at an air-water interface, including total internal reflection and Brewster-angle behavior.

References are suggested by the research engine and may be incomplete. Unverified URLs are omitted rather than guessed.

Article history

  1. Version 130 October 2026 · EditorCreated by Zapia