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NCERT Exemplar · Q29

Q.The mixture a pure liquid and a solution in a long vertical column (i.e, horizontal dimensions ≪\ll vertical dimensions) produces diffusion of solute particles and hence a refractive index gradient along the vertical dimension. A ray of light entering the column at right angles to the vertical is deviated from its original path. Find the deviation in travelling a horizontal distance d≪hd \ll h, the height of the column.

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A ray bends continuously in a medium with a vertical refractive index gradient. By treating the gradient as constant over the small horizontal distance dd, the deviation angle is θ≈dn0(dndy)\theta \approx \frac{d}{n_0} \left( \frac{dn}{dy} \right), where n0n_0 is the refractive index at the entry point and dndy\frac{dn}{dy} is the vertical gradient.

Why This Works: The Physics of Bending Light

When a ray of light enters a medium where the refractive index varies smoothly in a direction perpendicular to its path, the ray does not suddenly change direction at a single point — it curves continuously. This is the same principle that causes mirages and the twinkling of stars.

The key insight is Snell's law in differential form: for a ray moving through a medium with a gradient in refractive index, the local radius of curvature is determined by how fast nn changes across the ray's path. For small deviations, we can treat the bending as a gradual accumulation of tiny angular deflections.

Tip

Think of it like a car driving on a road that tilts sideways — the car drifts in the direction of the tilt. Here, the "tilt" is the refractive index gradient, and the "drift" is the bending of the light ray.

Step-by-Step Solution

1. Set up the geometry and the gradient

Let the vertical direction be yy (positive upward) and the horizontal direction be xx (the direction the ray initially travels). The refractive index varies only with yy: n=n(y)n = n(y). At the entry point, let y=y0y = y_0 and n(y0)=n0n(y_0) = n_0.

The ray enters horizontally, so initially the wavefront is vertical. As the ray moves a small horizontal distance dxdx, it encounters slightly different refractive indices at different heights.

2. Apply the differential form of Snell's law

For a ray in a medium with a gradient, the local curvature is given by:

1R=1ndndycos⁡θ\frac{1}{R} = \frac{1}{n} \frac{dn}{dy} \cos \theta

where θ\theta is the angle the ray makes with the horizontal. For small deviations, θ\theta is small, so cos⁡θ≈1\cos \theta \approx 1. The radius of curvature RR relates to the change in direction dθd\theta over a path length dsds by dθ=ds/Rd\theta = ds / R.

Since the ray is nearly horizontal, ds≈dxds \approx dx. Therefore:

dθ=dxR=1ndndy dxd\theta = \frac{dx}{R} = \frac{1}{n} \frac{dn}{dy} \, dx

3. Integrate over the horizontal distance

The ray travels a horizontal distance dd. Over this short distance, nn and dndy\frac{dn}{dy} change very little from their values at the entry point. So we can treat them as constants:

θ=∫0d1n0(dndy)y0dx=dn0(dndy)y0\theta = \int_0^d \frac{1}{n_0} \left( \frac{dn}{dy} \right)_{y_0} dx = \frac{d}{n_0} \left( \frac{dn}{dy} \right)_{y_0}

This θ\theta is the total deviation angle — the angle between the final direction of the ray and its original horizontal direction. …

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