Geometrical Optics

NEET Physics · 99 questions · Page 7 of 10 · Click an option or "Show Solution" to reveal answer

Q61
A ray of light travelling in a transparent medium of refractive index μ\mu , falls on a surface separating the medium from air at an angle of incidence of 45 o . For which of the following value of μ\mu the ray can undergo total internal reflection ?
A μ\mu = 1.33
B μ\mu = 1.40
C μ\mu = 1.50
D μ\mu = 1.25
Correct Answer
Option C
Solution

For total internal reflection, sini >> sinC where, i = angle of incidence, C = critical angle But, sinC =

1μ{1 \over \mu }

\therefore sini >>

1μ{1 \over \mu }

\Rightarrow μ\mu >>

1sini{1 \over {\sin i}}

\therefore μ\mu >>

1sin45{1 \over {\sin 45^\circ }}

\Rightarrow μ\mu >>

2\sqrt 2
Q62
A lens having focal length f and aperture of diameter d forms an image of intensity I. Aperture of diameter d2{d \over 2} in central region of lens is covered by a black paper. Focal length of lens and intensity of image now will be respectively
A ff\, and I4{I \over 4}
B 3f4{{3f} \over 4} and I2{I \over 2}
C ff and 3I4{{3I} \over 4}
D f2{f \over 2} and I2{I \over 2}
Correct Answer
Option C
Solution

By covering aperture, focal length does not change. But intensity is reduced by

14{1 \over 4}

times, as aperture diameter

d2{d \over 2}

is covered. \therefore I' = I -

I4{I \over 4}

=

3I4{{3I} \over 4}

\therefore New focal length = f and intensity =

3I4{{3I} \over 4}
Q63
Two thin lenses of focal lengths f 1 and f 2 are in contact and coaxial. The power of the combination is
A f1+f22{{{f_1} + {f_2}} \over 2}
B f1+f2f1f2{{{f_1} + {f_2}} \over {{f_1}{f_2}}}
C f1f2\sqrt {{{{f_1}} \over {{f_2}}}}
D f2f1\sqrt {{{{f_2}} \over {{f_1}}}}
Correct Answer
Option B
Solution
1f=1f1+1f2{1 \over f} = {1 \over {{f_1}}} + {1 \over {{f_2}}}

\therefore Power P =

f1+f2f1f2{{{f_1} + {f_2}} \over {{f_1}{f_2}}}
Q64
A boy is trying to start a fire by focusing sunlight on a piece of paper using an equiconvex lens of focal length 10 cm. The diameter of the sun is 1.39 × \times 10 9 m and its mean distance from the earth is 1.5 × \times 10 11 m. What is the diameter of the sun's image on the paper ?
A 6.5 × \times 10 -5 m
B 12.4 × \times 10 -4 m
C 9.2 × \times 10 -4 m
D 6.5 × \times 10 -4 m
Correct Answer
Option C
Solution
vu=\left| {{v \over u}} \right| =

size of image size of object Size of image =

vu\left| {{v \over u}} \right|

×\times Size of object =

(1011.5×1011)×(1.39×109)\left( {{{{{10}^{ - 1}}} \over {1.5 \times {{10}^{11}}}}} \right) \times \left( {1.39 \times {{10}^9}} \right)

= 9.2 ×10 –4 m \therefore Diameter of the sun’s image = 9.2 ×10 –4 m

Q65
A small coin is resting on the bottom of a beaker filled with liquid . A ray of light from the coin travels upto the surface of the liquid and moves along its surface. How fast is the light travelling in the liquid ?
A 2.4 × \times 10 8 m/s
B 3.0 × \times 10 8 m/s
C 1.2 × \times 10 8 m/s
D 1.8 × \times 10 8 m/s
Correct Answer
Option D
Solution

As

1μ=sinisin90{1 \over \mu } = {{\sin i} \over {\sin 90^\circ }}

\Rightarrow μ\mu =

1sini{1 \over {\sin i}}

=

53{5 \over 3}

Speed, v =

cμ{c \over \mu }

=

3×1085/3{{3 \times {{10}^8}} \over {5/3}}

= 1.8 ×\times 10 8 m/s

Q66
A convex lens and a concave lens, each having same focal length of 25 cm, are put in contact to form a combination of lenses. The power in diopters of the combination is
A zero
B 25
C 50
D infinite.
Correct Answer
Option A
Solution

Power of combination in dioptres P = P 1 + P 2 =

100f1{{100} \over {{f_1}}}

+

100f2{{100} \over {{f_2}}}

=

1002510025{{100} \over {25}} - {{100} \over {25}}

= 0

Q67
A microscope is focussed on a mark on a piece of paper and then a slab of glass of thickness 3 cm and refractive index 1.5 is placed over the mark. How should the microscope be moved to get the mark in focus again ?
A 2 cm upward
B 1 cm upward
C 4.5 cm downward
D 1 cm downward
Correct Answer
Option B
Solution

Apparent depth =

realdepthμ{{real\,depth} \over \mu }

=

31.5{3 \over {1.5}}

= 2 cm As image appears to be raised by 1 cm, therefore, microscope must be moved upwards by 1 cm.

Q68
A beam of light composed of red and green ray is incident obliquely at a point on the face of rectangular glass slab. When coming out on the opposite parallel face, the red green ray emerge from
A Two points propagating in two different non parallel directions
B Two points propagating in two different parallel directions.
C One point propagating in two different directions.
D One point propagating in the same firections.
Correct Answer
Option B
Solution

Red and green rays emerge from two points, propagating in two different parallel directions.

Q69
The refractive index of the material of a prism is 2\sqrt 2 and its refracting angle is 30 o . One of the refracting surfaces of the prism is made a mirror inwards. A beam of monochromatic light entering the prism from the other face with retrace its path after reflection from the mirrored surface if its angle of incidence on the prism is
A 45 o
B 60 o
C 0
D 30 o
Correct Answer
Option A
Solution

Using law of triangle, we get

r\angle r

= 30 o μ\mu =

sinisinr{{\sin i} \over {\sin r}}

\Rightarrow

2×sin30\sqrt 2 \times \sin 30^\circ

= sini \Rightarrow sini =

12{1 \over {\sqrt 2 }}

\Rightarrow i = 45 o

Q70
An equiconvex lens is cut into two halves along (i) XOX' and (ii) YOY' as shown in the figure. Let f,f,f,f', ff'' be the focal lengths of the complete lens, of each half in case (i), and of each half in case (ii), respectively. Choose the correct statement from the following
A f=f,f=2ff' = f,f'' = 2f
B f=2f,f=ff' = 2f,f'' = f
C f=f,f=ff' = f,f'' = f
D f=2f,f=2ff' = 2f,f'' = 2f
Correct Answer
Option A
Solution

We know from Lens maker's formula

1f=(μ1)(1R11R2){1 \over f} = \left( {\mu - 1} \right)\left( {{1 \over {{R_1}}} - {1 \over {{R_2}}}} \right)

Initially, Here R 1 = R and R 2 = –R by convection. \therefore

1f=(μ1)2R{1 \over f} = \left( {\mu - 1} \right){2 \over R}

\Rightarrow

12f=(μ1)1R{1 \over {2f}} = \left( {\mu - 1} \right){1 \over R}

If we cut the lens along XOX' then the two halves of the lens will be having the same radii of curvature and so, focal length f' = f .

But when we cut it along YOY' then, we will have R 1 = R but R 2 = \infty \therefore

1f=(μ1)(1R1){1 \over {f''}} = \left( {\mu - 1} \right)\left( {{1 \over R} - {1 \over \infty }} \right)

=

(μ1)1R\left( {\mu - 1} \right){1 \over R}

=

12f{1 \over {2f}}

\Rightarrow f'' = 2f

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