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Q.A ray of light is incident on a prism at an angle of 45∘45^\circ and passes symmetrically as shown in the figure. Calculate :

(a) the angle of minimum deviation,
(b) the refractive index of the material of the prism, and
(c) the angle of refraction at the point P.
Figure — CBSE 2022 55/4/1 Q10
Figure
CBSECBSE Class XII Board 2022Subjective· 3mImportance★★★★★
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For a prism with symmetric passage, the ray travels parallel to the base inside. Given A=60∘A=60^\circ and i=45∘i=45^\circ, the minimum deviation δm=30∘\delta_m=30^\circ, refractive index n=2n=\sqrt2, and the angle of refraction at P is 30∘30^\circ.

The key insight here is that the problem states the ray "passes symmetrically" through the prism. In prism optics, symmetric passage means the ray inside the prism travels parallel to the base. This is the defining condition for minimum deviation — and it's the single most powerful simplification you can use.

When a ray passes symmetrically, two things become true automatically: the angle of incidence equals the angle of emergence (i=ei=e), and the two angles of refraction inside the prism are equal (r1=r2r_1=r_2). The figure shows an equilateral prism, so the apex angle A=60∘A=60^\circ. With i=45∘i=45^\circ given, you have everything you need.

Figure — CBSE 2022 55/4/1 Q10
Figure — CBSE 2022 55/4/1 Q10

Let's work through each part.

  1. Find the angle of minimum deviation δm\delta_m

    For any prism, the deviation δ\delta is given by δ=i+e−A\delta = i + e - A. At minimum deviation, i=ei=e, so:

δm=2i−A\delta_m = 2i - A

Substituting i=45∘i=45^\circ and A=60∘A=60^\circ:

δm=2(45∘)−60∘=90∘−60∘=30∘\delta_m = 2(45^\circ) - 60^\circ = 90^\circ - 60^\circ = 30^\circ

Tip

The formula δm=2i−A\delta_m = 2i - A is only valid when the ray passes symmetrically (i.e., at minimum deviation). Don't use it for arbitrary incidence angles.

  1. Find the refractive index nn of the prism material

    The standard formula for refractive index at minimum deviation is:

n=sin⁡(A+δm2)sin⁡(A2)n = \frac{\sin\left(\frac{A+\delta_m}{2}\right)}{\sin\left(\frac{A}{2}\right)}

This formula comes from applying Snell's law at the first face and using the geometry r1=A/2r_1 = A/2 (which follows from r1=r2r_1=r_2 and r1+r2=Ar_1+r_2=A).

Plug in A=60∘A=60^\circ and δm=30∘\delta_m=30^\circ:

n=sin⁡(60∘+30∘2)sin⁡(60∘2)=sin⁡45∘sin⁡30∘n = \frac{\sin\left(\frac{60^\circ+30^\circ}{2}\right)}{\sin\left(\frac{60^\circ}{2}\right)} = \frac{\sin 45^\circ}{\sin 30^\circ}

Now sin⁡45∘=12\sin 45^\circ = \frac{1}{\sqrt{2}} and sin⁡30∘=12\sin 30^\circ = \frac{1}{2}, so:

n=1/21/2=22=2≈1.414n = \frac{1/\sqrt{2}}{1/2} = \frac{2}{\sqrt{2}} = \sqrt{2} \approx 1.414 …

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