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Question
Derive the equation for refraction at a single spherical surface.
Long Answer
Solution
- Let us consider two transparent media having refractive indices n1and n2 are separated by a spherical surface.
- Let C be the centre of curvature of the spherical surface. Let a point object O be in the medium n1.
- The line OC cuts the spherical surface at the pole P of the surface.
- As the rays considered are paraxial rays, the perpendicular dropped for the point of incidence to the principal axis is very close to the pole or passes through the pole itself.
- Light from O falls on the refracting surface at N. The normal drawn at the point of incidence passes through the centre of curvature C.
- As n2 > n1, light in the denser medium deviates towards the normal and meets the principal axis at I where the image is formed.
- By Snell’s law,
n1 sin i = n2 sin r
As the angles are small,
n1 i = n2 r
Let the angles,
∠ NOP = α, ∠ NCP = β ∠ NIP = γ
tan α = `"PN"/"PO"`;
tan β = `"PN"/"PC"`;
tan γ = `"PN"/"PI"` - As these angles are small, tan of angle could be approximated to the angle itself.
α = `"PN"/"PO"`;
β = `"PN"/"PC"`;
γ = `"PN"/"PI"`
for the triangle, ΔONC,
i = α + β
for the triangle, ΔINC,
β = r + γ (or) r = β – γ - on sub i & r, we get
n1 ( α + β) = n2 (β – γ)
Rearranging
n1α + n2γ = (n2 – n1)β
`"n"_1 ("PN"/"PO") + "n"_2 ("PN"/"PI") = ("n"_2 - "n"_1)("PN"/"PC")`
Further simplifying
`"n"_1/"PO" + "n"_2/"PI" = ("n"_2 - "n"_1)/"PC"`
`"n"_1/(-"u") + "n"_2/"v" = ("n"_2 - "n"_1)/"R"`
If the first medium is air then, n1 = 1 and
the second medium is taken just as n2 = n,
then the equation is reduced to.
`"n"/"v" - 1/"u" = ("n - 1")/"R"`
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Refraction at Single Spherical Surface
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