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QJEEAdv15Ph23f7: JEE Advanced 2015 Physics - Class 12 JEEAdv15Ph23f7 Solution: Consider a concave mirror and a convex lens (refractive index = …

Consider a concave mirror and a convex lens (refractive index = 1.5) of focal length 10 cm each, separated by a distance of 50 cm in air (refractive index = 1) as shown in the figure. An object is placed at a distance of 15 cm from the mirror. Its erect image formed by this combination has magnification M1. When the set-up is kept in a medium of refractive index 76{7 \over 6} , the magnification becomes M2. The magnitude ∣M2M1∣\left| {{{{M_2}} \over {{M_1}}}} \right| is
JEE Advanced 2015 Paper 1 Offline Physics - Geometrical Optics Question 39 English

Step-by-Step Verified Solution

Case I

Reflection from mirror

1f=1v+1u⇒1−10=1v+1−15{1 \over f} = {1 \over v} + {1 \over u} \Rightarrow {1 \over { - 10}} = {1 \over v} + {1 \over { - 15}}

⇒v=−30\Rightarrow v = - 30

JEE Advanced 2015 Paper 1 Offline Physics - Geometrical Optics Question 39 English Explanation

For lens 1f=1v−1u{1 \over f} = {1 \over v} - {1 \over u}

110=1v−1−20{1 \over {10}} = {1 \over v} - {1 \over { - 20}}

v=20v = 20

∣M1∣=∣v1u1∣∣v2u2∣\left| {{M_1}} \right| = \left| {{{{v_1}} \over {{u_1}}}} \right|\left| {{{{v_2}} \over {{u_2}}}} \right|

=(3015)(2020)= \left( {{{30} \over {15}}} \right)\left( {{{20} \over {20}}} \right)

=2×1=2= 2 \times 1 = 2 (in air)

Case II :

Now, consider the setup placed in a medium of refractive index μ1′{\mu {'_1}} = 7/6. The focal length of the mirror does not change. Thus, the distance of the image formed by the mirror and its magnification does not change. The focal length of the lens changes. The refractive index of the lens material is μ\mu 2 = 1.5. Apply lens maker's formula to get the new focal length of the lens

1f′=(μ2−μ1′μ1′)[1R1−1R2]{1 \over {f'}} = \left( {{{{\mu _2} - \mu {'_1}} \over {\mu {'_1}}}} \right)\left[ {{1 \over {{R_1}}} - {1 \over {{R_2}}}} \right]

=μ2−μ1′μ1′μ1μ2−μ1μ2−μ1μ1[1R1−1R2]= {{{\mu _2} - \mu {'_1}} \over {\mu {'_1}}}{{{\mu _1}} \over {{\mu _2} - {\mu _1}}}{{{\mu _2} - {\mu _1}} \over {{\mu _1}}}\left[ {{1 \over {{R_1}}} - {1 \over {{R_2}}}} \right]

=(μ2−μ1′μ2−μ1)(μ1μ1′)1f= \left( {{{{\mu _2} - \mu {'_1}} \over {{\mu _2} - {\mu _1}}}} \right)\left( {{{{\mu _1}} \over {\mu {'_1}}}} \right){1 \over f}

=(1.5−7/61.5−1)(17/6)110=235= \left( {{{1.5 - 7/6} \over {1.5 - 1}}} \right)\left( {{1 \over {7/6}}} \right){1 \over {10}} = {2 \over {35}} . ..... (1)

Again using lens formula, 1v−1u=1fl′{1 \over v} - {1 \over u} = {1 \over {{f_l}'}}

1v−1−20=235⇒1v=235−120=1140{1 \over v} - {1 \over { - 20}} = {2 \over {35}} \Rightarrow {1 \over v} = {2 \over {35}} - {1 \over {20}} = {1 \over {140}}

∴\therefore v = 140 cm

Magnification, m2′=vu=140−20=−7{m_2}' = {v \over u} = {{140} \over { - 20}} = - 7

Magnification produced by the combination,

M2=m1×m2′=(−2)×(−7)=14{M_2} = {m_1} \times {m_2}' = ( - 2) \times ( - 7) = 14

∴\therefore ∣M2M1∣=142=7\left| {{{{M_2}} \over {{M_1}}}} \right| = {{14} \over 2} = 7

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