derive the formula of refraction from rarer to denser medium at concave sperical refracting surface
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We have from Snell’s law −
μ =
sin i
sin r
From our assumptions made earlier we get −
sin i = i and sin r = r
Therefore,
i = μ r
From figure we can obtain −
i = α - γ and r = β - γ
∴ α - γ = μ(β - γ)
∴ α - γ = μβ - μγ
∴ α - μβ = γ(1 - μ)
Again using assumptions, we get −
∴ tan α - μ tan β = tan γ(1 - μ)
Suppose in figure point M is very close to P.
From figure −
tan α =
QM
OM
and tan β =
QM
IM
and tan γ =
QM
CM
Substituting values, we get −
QM
OM
- μ
QM
IM
=
QM
CM
(1 - μ)
Divide the equation by QM
1
OM
- μ
1
IM
=
1
CM
(1 - μ)
Substituting values of OM, IM, CM in optical terms from figure –
1
-u
- μ
1
-v
=
1
-R
(1 - μ)
∴
μ
v
-
1
u
= (μ - 1)
1
R
Where,
μ = Refractive index.
v = Image distance.
u = Object distance.
R = Radius of Curvature.
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