JEE Challenger
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Apparent Depth Comparison in Glass Cylindrical Media with Different Curved Surfaces

Consider three glass cylinders, each having an equal height H=30 cmH = 30\text{ cm} and refractive index n=1.5n = 1.5, resting on a horizontal base as shown in the diagram. Cylinder I has a flat upper surface, cylinder II has a convex upper surface, and cylinder III has a concave upper surface. The radius of curvature for both curved surfaces is R=3 mR = 3\text{ m}. Let H1H_1, H2H_2, and H3H_3 represent the apparent depths of a point XX located at the bottom of the three cylinders, respectively. Identify the correct statement(s):

Question Diagram 1

Options

A

H2>H1H_2 > H_1

Correct
B

H3>H1H_3 > H_1

C

H2>H3H_2 > H_3

Correct
D

0.8 cm<(H2−H1)<0.9 cm0.8\text{ cm} < (H_2 - H_1) < 0.9\text{ cm}

Step-by-Step Solution

To find the correct statements, we analyze the refraction of light at the top surface of each glass cylinder.

General Formula for Refraction at a Single Spherical Surface

The relation between object distance (uu), image distance (vv), refractive indices of the media, and radius of curvature (RR) is given by: n2v−n1u=n2−n1R\frac{n_2}{v} - \frac{n_1}{u} = \frac{n_2 - n_1}{R}

Sign Convention:

  • Light travels from point XX inside the glass (n1=1.5n_1 = 1.5) upwards into air (n2=1.0n_2 = 1.0). Therefore, the upward direction is positive.
  • The pole (vertex) of each top surface is taken as the origin.
  • The object XX is located below the top surface, so the object distance is: u=−H=−30 cmu = -H = -30\text{ cm}

1. Cylinder I (Flat Top Surface)

For a flat surface, the radius of curvature R→∞R \to \infty. Substituting the values into the refraction formula: 1v1−1.5−30=0\frac{1}{v_1} - \frac{1.5}{-30} = 0 1v1+120=0  ⟹  v1=−20 cm\frac{1}{v_1} + \frac{1}{20} = 0 \implies v_1 = -20\text{ cm}

Thus, the apparent depth H1H_1 is: H1=∣v1∣=20 cmH_1 = |v_1| = 20\text{ cm}


2. Cylinder II (Convex Top Surface)

For the convex upper surface, the center of curvature lies inside the glass (below the vertex). Since this direction is opposite to the upward path of incident light: R=−3 m=−300 cmR = -3\text{ m} = -300\text{ cm}

Applying the refraction formula: 1v2−1.5−30=1.0−1.5−300\frac{1}{v_2} - \frac{1.5}{-30} = \frac{1.0 - 1.5}{-300} 1v2+120=−0.5−300=1600\frac{1}{v_2} + \frac{1}{20} = \frac{-0.5}{-300} = \frac{1}{600} 1v2=1600−120=1−30600=−29600\frac{1}{v_2} = \frac{1}{600} - \frac{1}{20} = \frac{1 - 30}{600} = -\frac{29}{600} v2=−60029 cmv_2 = -\frac{600}{29}\text{ cm}

Thus, the apparent depth H2H_2 is: H2=∣v2∣=60029 cm≈20.69 cmH_2 = |v_2| = \frac{600}{29}\text{ cm} \approx 20.69\text{ cm}


3. Cylinder III (Concave Top Surface)

For the concave upper surface, the center of curvature lies in air (above the vertex), which is in the direction of the incident light: R=+3 m=+300 cmR = +3\text{ m} = +300\text{ cm}

Applying the refraction formula: 1v3−1.5−30=1.0−1.5+300\frac{1}{v_3} - \frac{1.5}{-30} = \frac{1.0 - 1.5}{+300} 1v3+120=−0.5300=−1600\frac{1}{v_3} + \frac{1}{20} = \frac{-0.5}{300} = -\frac{1}{600} 1v3=−1600−120=−1−30600=−31600\frac{1}{v_3} = -\frac{1}{600} - \frac{1}{20} = \frac{-1 - 30}{600} = -\frac{31}{600} v3=−60031 cmv_3 = -\frac{600}{31}\text{ cm}

Thus, the apparent depth H3H_3 is: H3=∣v3∣=60031 cm≈19.35 cmH_3 = |v_3| = \frac{600}{31}\text{ cm} \approx 19.35\text{ cm}


Analysis of Options:

  • Option A: Since H2=20.69 cmH_2 = 20.69\text{ cm} and H1=20 cmH_1 = 20\text{ cm}, we have H2>H1H_2 > H_1. (Correct)
  • Option B: Since H3=19.35 cmH_3 = 19.35\text{ cm} and H1=20 cmH_1 = 20\text{ cm}, we have H3<H1H_3 < H_1. (Incorrect)
  • Option C: Since H2=20.69 cmH_2 = 20.69\text{ cm} and H3=19.35 cmH_3 = 19.35\text{ cm}, we have H2>H3H_2 > H_3. (Correct)
  • Option D: Calculating the difference H2−H1H_2 - H_1: H2−H1=60029−20=2029 cm≈0.69 cmH_2 - H_1 = \frac{600}{29} - 20 = \frac{20}{29}\text{ cm} \approx 0.69\text{ cm} Since 0.69 cm<0.8 cm0.69\text{ cm} < 0.8\text{ cm}, this inequality is false. (Incorrect)

Correct Statements:

(A) and (C)