State Snell's law of reflection of light

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Snells law of reflection of light states that:

  1. The ratio os sine angle of incidence to sine angle of refraction is constant.
  2. Angle of incidence is not equal to angle of refraction.
  3. Angle of incidence is equal to angle of emergence.
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 Snells law of reflection of light states that:

  1. The ratio os sine angle of incidence to sine angle of refraction is constant. i.e. sin i/sin r = canstant
  2. Angle of incidence is not equal to angle of refraction.
  3. Angle of incidence is equal to angle of emergence.

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  Snell's law states that the ratio of the  SINES  of the angles of incidence and refraction is equivalent to the ratio of  VELOCITY (S) in the two media, or equivalent to the opposite ratio of the indices of refraction:

frac{sintheta_1}{sintheta_2} = frac{v_1}{v_2} = frac{n_2}{n_1}

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In optics and physics, Snell's law (also known as Descartes' law, the Snell–Descartes law, and the law of refraction) is a formula used to describe the relationship between the angles of incidence and refraction, when referring to light or other waves passing through a boundary between two different isotropic media, such as water and glass.

In optics, the law is used in ray tracing to compute the angles of incidence or refraction, and in experimental optics and gemology to find the refractive index of a material. The law is also satisfied in metamaterials, which allow light to be bent "backward" at a negative angle of refraction (negative refractive index).

Although named after Dutch astronomer Willebrord Snellius (1580-1626), the law was first accurately described by the Arab scientist Ibn Sahl of Baghdad, when in 984 he used the law to derive lens shapes that focus light with no geometric aberrations in the manuscript On Burning Mirrors and Lenses (984).[1][2].

Snell's law states that the ratio of the sines of the angles of incidence and refraction is equivalent to the ratio of phase velocities in the two media, or equivalent to the opposite ratio of the indices of refraction:

frac{sintheta_1}{sintheta_2} = frac{v_1}{v_2} = frac{n_2}{n_1}

with each θ as the angle measured from the normal, v as the velocity of light in the respective medium (SI units are meters per second, or m/s) and n as the refractive index (which is unitless) of the respective medium.

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