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Q.Draw the ray diagram showing refraction of monochromatic light through a glass prism of refraction angle A. Hence derive formula for refractive index μ of glass prism in terms of angle of prism and angle of minimum deviation. Also draw i-δ curve of prism. OR Using the ray diagram for refraction at a spherical convex surface separating two media μ₁ and μ₂ (μ₂ > μ₁), derive the relation μ₂/v − μ₁/u = (μ₂ − μ₁)/R, where the symbols used have their usual meanings.

Chhattisgarh CgbseCGBSE Intermediate Board 2019Subjective· 5mImportance★★★★★
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Figure — This single question requires drawing the ray diagram of refraction through a prism (and an i-delta curve); th
Figure — This single question requires drawing the ray diagram of refraction through a prism (and an i-delta curve); th

At minimum deviation, the ray passes symmetrically through the prism (r₁=r₂, i=e); combining geometry (A = r₁+r₂) and Snell's law gives μ=sin⁡A+δm2/sin⁡A2\mu = \sin\frac{A+\delta_m}{2}/\sin\frac A2.

Ray diagram (description): A monochromatic ray is incident on one refracting face of a prism of refracting angle AA at angle of incidence i1i_1. It refracts at the first face (bending towards the normal, entering the denser glass), travels through the prism, and refracts again at the second face (bending away from the normal on exit), emerging at angle i2=ei_2 = e. The angle of deviation δ\delta is the angle between the direction of the incident ray (extended) and the emergent ray.

Geometry: Using the angles r1r_1 and r2r_2 made by the refracted ray with the normals at the two faces, geometry of the prism gives:

A=r1+r2A = r_1 + r_2

and considering the deviations at each face,

δ=(i1−r1)+(i2−r2)=i1+i2−A\delta = (i_1 - r_1) + (i_2 - r_2) = i_1 + i_2 - A

Minimum deviation condition: As the angle of incidence is varied, δ\delta first decreases, reaches a minimum value δm\delta_m, and then increases. At this minimum, the ray passes symmetrically through the prism: i1=i2=ii_1 = i_2 = i, and correspondingly r1=r2=r=A/2r_1 = r_2 = r = A/2. At this condition:

δm=2i−A⇒i=A+δm2\delta_m = 2i - A \quad \Rightarrow \quad i = \dfrac{A+\delta_m}{2}

Applying Snell's law at the first face, μ=sin⁡isin⁡r\mu = \dfrac{\sin i}{\sin r}, with r=A/2r = A/2:

μ=sin⁡(A+δm2)sin⁡(A2)\mu = \dfrac{\sin\left(\dfrac{A+\delta_m}{2}\right)}{\sin\left(\dfrac{A}{2}\right)}

i–δ curve: Plotting the angle of deviation δ\delta (y-axis) against the angle of incidence ii (x-axis) gives a roughly U-shaped curve: δ\delta is large for small ii, decreases as ii increases, reaches a single minimum value δm\delta_m at one particular angle of incidence (where the ray passes symmetrically, i=ei=e), and then increases again as ii increases further. The curve is (nearly) symmetric about this minimum point.

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