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Geometrical Optics question

2015 · Shift 2 · Q48
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Geometrical Optics question

2015 · Shift 2 · Q48

JEE AdvancedPhysicsGeometrical OpticsNumerical+4 / −1
A monochromatic beam of light is incident at 60 ∘^\circ∘ on one face of an equilateral prism of refractive index n and emerges from the opposite face making an angle θ\thetaθ(n) with the normal (see figure). For n = 3\sqrt 33​ the value of θ\thetaθ is 60 ∘^\circ∘ and dθdn=m{{d\theta } \over {dn}} = mdndθ​=m. The value of m is JEE Advanced 2015 Paper 2 Offline Physics - Geometrical Optics Question 46 English
Numerical answer
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Correct answer: 2

The user wants me to solve a physics problem about light passing through a prism and find the rate of change of the angle of emergence with respect to the refractive index.

1. Identify the given information and relevant equations:

  • Angle of incidence, i1=60∘i_1 = 60^\circi1​=60∘.
  • The prism is equilateral, so the angle of the prism, A=60∘A = 60^\circA=60∘.
  • The refractive index of the prism is nnn.
  • The angle of emergence is θ(n)\theta(n)θ(n).
  • We are given a specific case: when n=3n = \sqrt{3}n=3​, the angle of emergence is θ=60∘\theta = 60^\circθ=60∘.
  • We need to find m=dθdnm = \frac{d\theta}{dn}m=dndθ​ at this specific condition.

The behavior of light passing through the prism is described by Snell's law at the two faces and the geometry of the prism:

  • First face (incidence): 1⋅sin⁡i1=nsin⁡r11 \cdot \sin i_1 = n \sin r_11⋅sini1​=nsinr1​
  • Second face (emergence): nsin⁡r2=1⋅sin⁡θn \sin r_2 = 1 \cdot \sin \thetansinr2​=1⋅sinθ
  • Prism geometry: A=r1+r2A = r_1 + r_2A=r1​+r2​

where r1r_1r1​ is the angle of refraction at the first face and r2r_2r2​ is the angle of incidence at the second face.

2. Analyze the specific case (n=3n = \sqrt{3}n=3​): Let's find the values of r1r_1r1​ and r2r_2r2​ for this case.

  • Using Snell's law at the first face with i1=60∘i_1 = 60^\circi1​=60∘ and n=3n = \sqrt{3}n=3​: sin⁡60∘=3sin⁡r1\sin 60^\circ = \sqrt{3} \sin r_1sin60∘=3​sinr1​ 32=3sin⁡r1\frac{\sqrt{3}}{2} = \sqrt{3} \sin r_123​​=3​sinr1​ sin⁡r1=12  ⟹  r1=30∘\sin r_1 = \frac{1}{2} \implies r_1 = 30^\circsinr1​=21​⟹r1​=30∘

  • Using the prism geometry equation with A=60∘A = 60^\circA=60∘: r2=A−r1=60∘−30∘=30∘r_2 = A - r_1 = 60^\circ - 30^\circ = 30^\circr2​=A−r1​=60∘−30∘=30∘

  • We can verify this with Snell's law at the second face, given θ=60∘\theta = 60^\circθ=60∘: nsin⁡r2=3sin⁡30∘=3⋅12=32n \sin r_2 = \sqrt{3} \sin 30^\circ = \sqrt{3} \cdot \frac{1}{2} = \frac{\sqrt{3}}{2}nsinr2​=3​sin30∘=3​⋅21​=23​​ sin⁡θ=sin⁡60∘=32\sin \theta = \sin 60^\circ = \frac{\sqrt{3}}{2}sinθ=sin60∘=23​​ The values are consistent. This condition, where i1=θi_1=\thetai1​=θ and r1=r2r_1=r_2r1​=r2​, corresponds to the minimum deviation condition.

3. Find the derivative dθdn\frac{d\theta}{dn}dndθ​: We will differentiate the three prism equations with respect to nnn. Remember that r1r_1r1​, r2r_2r2​, and θ\thetaθ are all functions of nnn, while i1i_1i1​ and AAA are constants.

  • Differentiating sin⁡i1=nsin⁡r1\sin i_1 = n \sin r_1sini1​=nsinr1​: 0=ddn(nsin⁡r1)=1⋅sin⁡r1+ncos⁡r1dr1dn0 = \frac{d}{dn}(n \sin r_1) = 1 \cdot \sin r_1 + n \cos r_1 \frac{dr_1}{dn}0=dnd​(nsinr1​)=1⋅sinr1​+ncosr1​dndr1​​ dr1dn=−sin⁡r1ncos⁡r1=−tan⁡r1n\frac{dr_1}{dn} = -\frac{\sin r_1}{n \cos r_1} = -\frac{\tan r_1}{n}dndr1​​=−ncosr1​sinr1​​=−ntanr1​​

  • Differentiating r1+r2=Ar_1 + r_2 = Ar1​+r2​=A: dr1dn+dr2dn=0  ⟹  dr2dn=−dr1dn=tan⁡r1n\frac{dr_1}{dn} + \frac{dr_2}{dn} = 0 \implies \frac{dr_2}{dn} = -\frac{dr_1}{dn} = \frac{\tan r_1}{n}dndr1​​+dndr2​​=0⟹dndr2​​=−dndr1​​=ntanr1​​

  • Differentiating nsin⁡r2=sin⁡θn \sin r_2 = \sin \thetansinr2​=sinθ: 1⋅sin⁡r2+ncos⁡r2dr2dn=cos⁡θdθdn1 \cdot \sin r_2 + n \cos r_2 \frac{dr_2}{dn} = \cos \theta \frac{d\theta}{dn}1⋅sinr2​+ncosr2​dndr2​​=cosθdndθ​

Now, substitute the expression for dr2dn\frac{dr_2}{dn}dndr2​​ into the last equation: sin⁡r2+ncos⁡r2(tan⁡r1n)=cos⁡θdθdn\sin r_2 + n \cos r_2 \left(\frac{\tan r_1}{n}\right) = \cos \theta \frac{d\theta}{dn}sinr2​+ncosr2​(ntanr1​​)=cosθdndθ​ sin⁡r2+cos⁡r2tan⁡r1=cos⁡θdθdn\sin r_2 + \cos r_2 \tan r_1 = \cos \theta \frac{d\theta}{dn}sinr2​+cosr2​tanr1​=cosθdndθ​ sin⁡r2+cos⁡r2sin⁡r1cos⁡r1=cos⁡θdθdn\sin r_2 + \cos r_2 \frac{\sin r_1}{\cos r_1} = \cos \theta \frac{d\theta}{dn}sinr2​+cosr2​cosr1​sinr1​​=cosθdndθ​ sin⁡r2cos⁡r1+cos⁡r2sin⁡r1cos⁡r1=cos⁡θdθdn\frac{\sin r_2 \cos r_1 + \cos r_2 \sin r_1}{\cos r_1} = \cos \theta \frac{d\theta}{dn}cosr1​sinr2​cosr1​+cosr2​sinr1​​=cosθdndθ​

Using the trigonometric identity sin⁡(x+y)=sin⁡xcos⁡y+cos⁡xsin⁡y\sin(x+y) = \sin x \cos y + \cos x \sin ysin(x+y)=sinxcosy+cosxsiny: sin⁡(r1+r2)cos⁡r1=cos⁡θdθdn\frac{\sin(r_1 + r_2)}{\cos r_1} = \cos \theta \frac{d\theta}{dn}cosr1​sin(r1​+r2​)​=cosθdndθ​

Since r1+r2=Ar_1 + r_2 = Ar1​+r2​=A: sin⁡Acos⁡r1=cos⁡θdθdn\frac{\sin A}{\cos r_1} = \cos \theta \frac{d\theta}{dn}cosr1​sinA​=cosθdndθ​

Solving for dθdn\frac{d\theta}{dn}dndθ​: dθdn=sin⁡Acos⁡r1cos⁡θ\frac{d\theta}{dn} = \frac{\sin A}{\cos r_1 \cos \theta}dndθ​=cosr1​cosθsinA​

4. Calculate the value of mmm: We need to evaluate this derivative at the given condition: n=3n = \sqrt{3}n=3​. From step 2, we have the corresponding angles:

  • A=60∘A = 60^\circA=60∘
  • r1=30∘r_1 = 30^\circr1​=30∘
  • θ=60∘\theta = 60^\circθ=60∘

Substitute these values into the expression for the derivative: m=dθdn∣n=3=sin⁡60∘cos⁡30∘cos⁡60∘m = \frac{d\theta}{dn} \bigg|_{n=\sqrt{3}} = \frac{\sin 60^\circ}{\cos 30^\circ \cos 60^\circ}m=dndθ​​n=3​​=cos30∘cos60∘sin60∘​ m=32(32)(12)m = \frac{\frac{\sqrt{3}}{2}}{\left(\frac{\sqrt{3}}{2}\right) \left(\frac{1}{2}\right)}m=(23​​)(21​)23​​​ m=112=2m = \frac{1}{\frac{1}{2}} = 2m=21​1​=2

The value of m is 2.

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