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Question: A particle is moving in front of a thin equi-convex lens of radius of curvature 10 cm and refractive...

A particle is moving in front of a thin equi-convex lens of radius of curvature 10 cm and refractive index 43\frac{4}{3}. Figure shows an instant when the particle is making 60° with the principal axis and its image is making 30° with the axis. List-I mentions some quantities at the instant shown and List-II mentions their corresponding values.

A

Distance of object from lens is (in cm)

B

Distance of image from lens is (in cm)

C

Magnitude of magnification is

D

 Velocity of image Velocity of object\frac{\text { Velocity of image}}{\text { Velocity of object}}

E

40

F

3

G

20

H

333\sqrt{3}

I

60

Answer

P-3, Q-5, R-2, S-4

Explanation

Solution

To solve this problem, we need to calculate the focal length of the lens, then use the relationship between the object and image velocities to find the magnification, and finally use the lens formula to determine object and image distances.

1. Calculate the focal length (f) of the equi-convex lens: Given: Radius of curvature R=10R = 10 cm, refractive index μ=43\mu = \frac{4}{3}. For an equi-convex lens, R1=+R=+10R_1 = +R = +10 cm and R2=R=10R_2 = -R = -10 cm. Using the lens maker's formula: 1f=(μ1)(1R11R2)\frac{1}{f} = (\mu - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) 1f=(431)(110110)\frac{1}{f} = \left(\frac{4}{3} - 1\right) \left( \frac{1}{10} - \frac{1}{-10} \right) 1f=(13)(110+110)\frac{1}{f} = \left(\frac{1}{3}\right) \left( \frac{1}{10} + \frac{1}{10} \right) 1f=(13)(210)=115\frac{1}{f} = \left(\frac{1}{3}\right) \left( \frac{2}{10} \right) = \frac{1}{15} So, the focal length of the lens is f=15f = 15 cm.

2. Determine the transverse magnification (mTm_T): Let vOv_O be the speed of the object and vIv_I be the speed of the image. The object's velocity components are: vOx=vOcos60v_{Ox} = v_O \cos 60^\circ (longitudinal component) vOy=vOsin60v_{Oy} = v_O \sin 60^\circ (transverse component)

The image's velocity components are: vIx=vIcos30v_{Ix} = v_I \cos 30^\circ (longitudinal component) vIy=vIsin30v_{Iy} = v_I \sin 30^\circ (transverse component)

For a lens, the relationship between longitudinal velocity components is vIx=mT2vOxv_{Ix} = m_T^2 v_{Ox} and for transverse velocity components is vIy=mTvOyv_{Iy} = m_T v_{Oy}. However, we need to be careful with signs. A real image formed by a convex lens is inverted, so mTm_T is negative. Let's consider the directions from the diagram. The object is approaching the lens (negative x-direction for vOxv_{Ox}) and moving upwards (positive y-direction for vOyv_{Oy}). The image is moving away from the lens (positive x-direction for vIxv_{Ix}) and downwards (negative y-direction for vIyv_{Iy}).

So, vOx=vOcos60v_{Ox} = -v_O \cos 60^\circ and vOy=vOsin60v_{Oy} = v_O \sin 60^\circ. And vIx=vIcos30v_{Ix} = v_I \cos 30^\circ and vIy=vIsin30v_{Iy} = -v_I \sin 30^\circ.

Using the relations: (1) vIy=mTvOy    vIsin30=mT(vOsin60)v_{Iy} = m_T v_{Oy} \implies -v_I \sin 30^\circ = m_T (v_O \sin 60^\circ) (2) vIx=mT2vOx    vIcos30=mT2(vOcos60)v_{Ix} = m_T^2 v_{Ox} \implies v_I \cos 30^\circ = m_T^2 (-v_O \cos 60^\circ)

From (1): vIvO=mTsin60sin30=mT3/21/2=mT3\frac{v_I}{v_O} = -m_T \frac{\sin 60^\circ}{\sin 30^\circ} = -m_T \frac{\sqrt{3}/2}{1/2} = -m_T \sqrt{3} From (2): vIvO=mT2cos60cos30=mT21/23/2=mT23\frac{v_I}{v_O} = -m_T^2 \frac{\cos 60^\circ}{\cos 30^\circ} = -m_T^2 \frac{1/2}{\sqrt{3}/2} = -\frac{m_T^2}{\sqrt{3}}

Equating the two expressions for vIvO\frac{v_I}{v_O}: mT3=mT23-m_T \sqrt{3} = -\frac{m_T^2}{\sqrt{3}} Since mT0m_T \neq 0, we can divide by mT-m_T: 3=mT3\sqrt{3} = \frac{m_T}{\sqrt{3}} mT=3m_T = 3 This result for mTm_T is positive, which implies an erect image. However, for a real image formed by a convex lens, the image is inverted, meaning mTm_T should be negative. The angular relationship implies the ratio of speeds is positive, but the actual mTm_T should be negative. The "magnitude of magnification" is asked in (R). So, mT=3|m_T| = 3. This matches with List-II (2).

3. Calculate object and image distances (u and v): Let uu be the object position and vv be the image position. By convention, uu is negative and vv is positive for a real image. The transverse magnification is mT=vum_T = \frac{v}{u}. Since the image is real and inverted, mT=3m_T = -3. So, vu=3    v=3u\frac{v}{u} = -3 \implies v = -3u.

Using the lens formula: 1v1u=1f\frac{1}{v} - \frac{1}{u} = \frac{1}{f} Substitute v=3uv = -3u and f=15f = 15 cm: 13u1u=115\frac{1}{-3u} - \frac{1}{u} = \frac{1}{15} 133u=115\frac{-1 - 3}{3u} = \frac{1}{15} 43u=115\frac{-4}{3u} = \frac{1}{15} 3u=4×153u = -4 \times 15 3u=603u = -60 u=20 cmu = -20 \text{ cm} The distance of the object from the lens is u=20|u| = 20 cm. This matches with List-II (3).

Now calculate vv: v=3u=3(20)=60 cmv = -3u = -3(-20) = 60 \text{ cm} The distance of the image from the lens is v=60|v| = 60 cm. This matches with List-II (5).

4. Calculate the ratio of velocities  Velocity of image Velocity of object\frac{\text { Velocity of image}}{\text { Velocity of object}}: Using the expression derived earlier: vIvO=mT3\frac{v_I}{v_O} = -m_T \sqrt{3} Substitute mT=3m_T = -3: vIvO=(3)3=33\frac{v_I}{v_O} = -(-3) \sqrt{3} = 3\sqrt{3} This matches with List-II (4).

Summary of matches:

  • (P) Distance of object from lens is (in cm) \rightarrow 20 (List-II (3))
  • (Q) Distance of image from lens is (in cm) \rightarrow 60 (List-II (5))
  • (R) Magnitude of magnification is \rightarrow 3 (List-II (2))
  • (S)  Velocity of image Velocity of object\frac{\text { Velocity of image}}{\text { Velocity of object}} \rightarrow 333\sqrt{3} (List-II (4))

The question is a matching type, and all options are uniquely matched.