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Refraction at a Thin Lens.

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Fig. shows a convex lens of a material of refractive index μ2 . The media on the two sides of the lens have refractive index μ1 and μ3 respectively. P is a point object placed on principal axis in medium 1 known as object space. PA is incident ray on the first surface of lens. Had there been only one surface the refracted ray AB would have met principal axis at Q1 . For refraction at first surface

From refraction formula at a spherical surface

The refracted ray AB from first surface meets second surface of lens at B and the emergent ray BQ meets principal axis at Q. Q is final image formed by lens due to refraction at both surfaces. For refraction at second surface of lens Q1 acts as a virtual object forming real image Q. For refraction at second surface

Adding Eqn. (1) and (2) we have

Let u and v denote the position of object P and final image Q. In terms of co–ordinate convention of signs.

u = –a; v = +b; R1 = +c; R2 = –d

We rewrite Eqn. (3) as

Equation (4) in the refraction formula for a thin lens. Commonly the media on both sides of lens is same i.e. μ1 = μ3 Eqn. (4) reduces to

This is refraction formula for a thin lens.

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