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Question #43182

Difficulty: 8/10 | 🟢 Free

The Question

A small object is placed at the bottom of a transparent liquid of depth HH (in m\text{m}). The refractive index of the liquid varies with depth yy (in m\text{m}) from the surface (y=0y=0) as n(y)=n02+αyn(y) = \sqrt{n_0^2 + \alpha y}, where n0n_0 is a dimensionless positive constant and α\alpha is a positive constant in m−1\text{m}^{-1}. An observer in air (nair=1n_{air} = 1) looks at the object such that the emergent ray entering their eye makes an angle θ0\theta_0 with the normal to the surface. The apparent depth H′H' is defined as the depth at which the backward-extended emergent ray intersects the vertical line passing through the actual object. Which of the following expressions gives H′H'?

Options

  • A.

    2cos⁡θ0α(n02−sin⁡2θ0+αH−n02−sin⁡2θ0)\frac{2\cos\theta_0}{\alpha} \left( \sqrt{n_0^2 - \sin^2\theta_0 + \alpha H} - \sqrt{n_0^2 - \sin^2\theta_0} \right)

  • B.

    Hcos⁡θ0n02−sin⁡2θ0\frac{H \cos\theta_0}{\sqrt{n_0^2 - \sin^2\theta_0}}

  • C.

    cos⁡θ0α(n02−sin⁡2θ0+αH−n02−sin⁡2θ0)\frac{\cos\theta_0}{\alpha} \left( \sqrt{n_0^2 - \sin^2\theta_0 + \alpha H} - \sqrt{n_0^2 - \sin^2\theta_0} \right)

  • D.

    Hcos⁡θ0n02+αH−sin⁡2θ0\frac{H \cos\theta_0}{\sqrt{n_0^2 + \alpha H - \sin^2\theta_0}}

Check Your Answer

Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Intuition_Breaker

Train your brain to resist "obvious" answers that are designed to deceive your intuition.

Concepts Behind This Question

Medium Dependency|Apparent Depth/Shift|Vector Decomposition Ambiguity|Approximations

Why This Question Is Tricky

Common Mistakes

Students often incorrectly assume that apparent depth formulas derived for constant refractive indices can be applied to gradient-index media by simply substituting the boundary refractive index values.

This trap tests the misapplication of Snell's Law as a linear, single-interface phenomenon rather than a continuous path integral.

By assuming the ray travels in a straight line and using either the surface index n0n_0 or the bottom index n02+αH\sqrt{n_0^2+\alpha H}, students fail to account for the continuous curvature of the ray path.

The correct approach requires applying the generalized Snell's Law to find the local slope of the ray, integrating this slope over the depth to find the true lateral displacement, and then using geometry to find the apparent depth.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterElectromagnetic Waves - Class 12
ConceptMedium Dependency
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree