Geometrical Optics

JEE Physics · 130 questions · Page 8 of 13 · Click an option or "Show Solution" to reveal answer

Q71
The critical angle for a denser-rarer interface is 4545^{\circ}. The speed of light in rarer medium is 3×108 m/s3 \times 10^{8} \mathrm{~m} / \mathrm{s}. The speed of light in the denser medium is:
A 2.12×108 m/s2 .12 \times 10^{8} \mathrm{~m} / \mathrm{s}
B 5×107 m/s5 \times 10^{7} \mathrm{~m} / \mathrm{s}
C 2×108 m/s\sqrt{2} \times 10^{8} \mathrm{~m} / \mathrm{s}
D 3.12×107 m/s3.12 \times 10^{7} \mathrm{~m} / \mathrm{s}
Correct Answer
Option A
Solution

To find the speed of light in the denser medium, we can use Snell's Law at the critical angle, where the angle of refraction is

9090^{\circ}

. Snell's Law states:

n1sinθ1=n2sinθ2n_1 \sin{\theta_1} = n_2 \sin{\theta_2}

where

n1n_1

and

n2n_2

are the indices of refraction for the denser and rarer media, respectively, and

θ1\theta_1

and

θ2\theta_2

are the angles of incidence and refraction, respectively. In this case, we have:

n1sin45=n2sin90n_1 \sin{45^{\circ}} = n_2 \sin{90^{\circ}}

The critical angle is given as

4545^{\circ}

, and the speed of light in the rarer medium is given as

3×108 m/s3 \times 10^8 \mathrm{~m/s}

. We can find the index of refraction of the rarer medium using the formula:

n=cvn = \frac{c}{v}

where

cc

is the speed of light in a vacuum (

3×108 m/s3 \times 10^8 \mathrm{~m/s}

), and

vv

is the speed of light in the medium. For the rarer medium, we have:

n2=3×108 m/s3×108 m/s=1n_2 = \frac{3 \times 10^8 \mathrm{~m/s}}{3 \times 10^8 \mathrm{~m/s}} = 1

Now we can rewrite Snell's Law as:

n1sin45=11n_1 \sin{45^{\circ}} = 1 \cdot 1
n1sin45=1n_1 \sin{45^{\circ}} = 1
n1=1sin45n_1 = \frac{1}{\sin{45^{\circ}}}

Since

sin45=12\sin{45^{\circ}} = \frac{1}{\sqrt{2}}

, we have:

n1=112=2n_1 = \frac{1}{\frac{1}{\sqrt{2}}} = \sqrt{2}

Now, we can find the speed of light in the denser medium using the formula for the index of refraction:

v1=cn1v_1 = \frac{c}{n_1}
v1=3×108 m/s2v_1 = \frac{3 \times 10^8 \mathrm{~m/s}}{\sqrt{2}}
v1=2.12×108 m/sv_1 = 2.12 \times 10^8 \mathrm{~m/s}

So, the speed of light in the denser medium is

2.12×108 m/s2.12 \times 10^8 \mathrm{~m/s}

.

Q72
An object is placed at a distance of 12 cm in front of a plane mirror. The virtual and erect image is formed by the mirror. Now the mirror is moved by 4 cm towards the stationary object. The distance by which the position of image would be shifted, will be
A 4 cm towards mirror
B 2 cm towards mirror
C 8 cm away from mirror
D 8 cm towards mirror
Correct Answer
Option D
Solution

\therefore Shifting of image will be 8 cm towards mirror.

Q73
In a reflecting telescope, a secondary mirror is used to:
A make chromatic aberration zero
B remove spherical aberration
C reduce the problem of mechanical support
D move the eyepiece outside the telescopic tube
Correct Answer
Option D
Solution

Reflecting telescopes, also known as reflectors, use a set of mirrors instead of lenses to gather and focus light.

The primary mirror (usually a concave mirror) gathers the incoming light and reflects it to a focus point.

The secondary mirror is used to redirect this focused light out to where it can be conveniently observed.

In other words, the secondary mirror in a reflecting telescope is used to move the eyepiece outside the telescopic tube, where the image can be comfortably viewed.

This is especially important for large telescopes, where the focus point may be inside the telescope tube and inaccessible without a secondary mirror.

Q74
A monochromatic light wave with wavelength λ1\lambda_{1} and frequency v1v_{1} in air enters another medium. If the angle of incidence and angle of refraction at the interface are 4545^{\circ} and 3030^{\circ} respectively, then the wavelength λ2\lambda_{2} and frequency v2v_{2} of the refracted wave are:
A λ2=λ1,v2=12v1\lambda_{2}=\lambda_{1}, v_{2}=\dfrac{1}{\sqrt{2}} v_{1}
B λ2=λ1,v2=2v1\lambda_{2}=\lambda_{1}, v_{2}=\sqrt{2} v_{1}
C λ2=2λ1,v2=v1\lambda_{2}=\sqrt{2} \lambda_{1}, v_{2}=v_{1}
D λ2=12λ1,v2=v1\lambda_{2}=\dfrac{1}{\sqrt{2}} \lambda_{1}, v_{2}=v_{1}
Correct Answer
Option D
Solution

When a light wave moves from one medium to another, its speed and wavelength may change, but its frequency remains constant because it is determined by the source of the light.

This is because frequency depends on the oscillations of the source, which do not change when entering a different medium.

Snell's law, which describes the relationship between the angles of incidence and refraction, can be written as: n1sin(θ1)=n2sin(θ2), n_1 \sin(\theta_1) = n_2 \sin(\theta_2), where n1n_1 and n2n_2 are the refractive indices of the two media, and θ1\theta_1 and θ2\theta_2 are the angles of incidence and refraction, respectively.

The refractive index of a medium is also related to the speed of light in that medium: n=cv, n = \dfrac{c}{v}, where cc is the speed of light in a vacuum, and vv is the speed of light in the medium.

From the above relations, we see that as light enters a medium with a higher refractive index (and hence a lower speed), its wavelength decreases.

The frequency remains the same.

Given that the angle of incidence is 4545^\circ and the angle of refraction is 3030^\circ, the ratio of the refractive indices is: n2n1=sin(θ1)sin(θ2)=sin(45)sin(30)=2. \dfrac{n_2}{n_1} = \dfrac{\sin(\theta_1)}{\sin(\theta_2)} = \dfrac{\sin(45^\circ)}{\sin(30^\circ)} = \sqrt{2}. This indicates that the speed of light (and hence the wavelength) decreases by a factor of 2\sqrt{2} as it enters the second medium.

The frequency remains the same.

Therefore, the correct answer is λ2=12λ1,v2=v1. \lambda_2 = \dfrac{1}{\sqrt{2}} \lambda_1, \quad v_2 = v_1.

Q75
Identify the physical quantity that cannot be measured using spherometer :
A Radius of curvature of concave surface
B Specific rotation of liquids
C Thickness of thin plates
D Radius of curvature of convex surface
Correct Answer
Option B
Solution

Spherometer can be used to measure curvature of surface.

Q76
The refractive index of a prism with apex angle AA is cotA/2\cot A / 2. The angle of minimum deviation is :
A δm=1803 A\delta_m=180^{\circ}-3 \mathrm{~A}
B δm=1804A\delta_m=180^{\circ}-4 A
C δm=1802A\delta_m=180^{\circ}-2 A
D δm=180A\delta_m=180^{\circ}-A
Correct Answer
Option C
Solution
μ=sin(A+δm2)sinA2cosA2sinA2=sin(A+δm2)sinA2sin(π2A2)=sin(A+δm2)π2A2=A2+δm2δm=π2A\begin{aligned} & \mu=\frac{\sin \left(\frac{A+\delta m}{2}\right)}{\sin \frac{A}{2}} \\ & \frac{\cos \frac{A}{2}}{\sin \frac{A}{2}}=\frac{\sin \left(\frac{A+\delta m}{2}\right)}{\sin \frac{A}{2}} \\ & \sin \left(\frac{\pi}{2}-\frac{A}{2}\right)=\sin \left(\frac{A+\delta_m}{2}\right) \\ & \frac{\pi}{2}-\frac{A}{2}=\frac{A}{2}+\frac{\delta m}{2} \\ & \delta_m=\pi-2 A \end{aligned}
Q77
A convex mirror of radius of curvature 30 cm30 \mathrm{~cm} forms an image that is half the size of the object. The object distance is :
A -45 cm
B -15 cm
C 45 cm
D 15 cm
Correct Answer
Option B
Solution

Given

R=30 cm\mathrm{R}=30 \mathrm{~cm}
f=R/2=+15 cm\mathrm{f}=\mathrm{R} / 2=+15 \mathrm{~cm}

Magnification

(m)=±12(\mathrm{m})= \pm \frac{1}{2}

For convex mirror, virtual image is formed for real object. Therefore,

m\mathrm{m}

is +ve

12=ffuu=15 cm\begin{aligned} & \frac{1}{2}=\frac{f}{f-u} \\ & u=-15 \mathrm{~cm} \end{aligned}
Q78
A biconvex lens of refractive index 1.5 has a focal length of 20 cm20 \mathrm{~cm} in air. Its focal length when immersed in a liquid of refractive index 1.6 will be:
A -16 cm
B +16 cm
C +160 cm
D -160 cm
Correct Answer
Option D
Solution
μ1=1.5μm=1.6fa=20 cm As fmfa=(μ11)μm(μ1μm)fm20=(1.51)1.6(1.51.6)fm=160 cm\begin{aligned} & \mu_1=1.5 \\ & \mu_m=1.6 \\ & f_a=20 \mathrm{~cm} \\ & \text{ As } \frac{f_m}{f_a}=\frac{\left(\mu_1-1\right) \mu_m}{\left(\mu_1-\mu_m\right)} \\ & \frac{f_m}{20}=\frac{(1.5-1) 1.6}{(1.5-1.6)} \\ & f_m=-160 \mathrm{~cm} \end{aligned}
Q79
If the distance between object and its two times magnified virtual image produced by a curved mirror is 15 cm15 \mathrm{~cm}, the focal length of the mirror must be:
A 10-10 cm
B 12-12 cm
C 15 cm
D 10/3 cm
Correct Answer
Option A
Solution
m=2=vu2=(15u)u2u=15u3u=15u=5 cmv=15u=155=10 cm1f=1v+1u=110+1(5)=1210=110f=10 cm\begin{aligned} & \mathrm{m}=2=\frac{-v}{u} \\ & 2=\frac{-(15-u)}{-u} \\ & 2 u=15-u \\ & 3 u=15 \Rightarrow u=5 \mathrm{~cm} \\ & v=15-u=15-5=10 \mathrm{~cm} \\ & \frac{1}{f}=\frac{1}{v}+\frac{1}{u} \\ & =\frac{1}{10}+\frac{1}{(-5)}=\frac{1-2}{10}=\frac{-1}{10} \\ & f=-10 \mathrm{~cm} \end{aligned}
Q80
Given below are two statements : Statement (I) : When an object is placed at the centre of curvature of a concave lens, image is formed at the centre of curvature of the lens on the other side. Statement (II) : Concave lens always forms a virtual and erect image. In the light of the above statements, choose the correct answer from the options given below :
A Statement I is false but Statement II is true
B Both Statement I and Statement II are false
C Both Statement I and Statement II are true
D Statement I is true but Statement II is false
Correct Answer
Option A
Solution

Let's analyze each statement carefully: Statement (I): When an object is placed at the centre of curvature of a concave lens, image is formed at the centre of curvature of the lens on the other side.

To understand this statement, let's recall the nature of images formed by concave lenses.

A concave lens (diverging lens) always forms images that are virtual, erect, and smaller than the object, regardless of the object's position.

The term "centre of curvature" is typically associated with mirrors rather than lenses.

Therefore, this statement is incorrect because a concave lens does not form a real image that could be said to be at the centre of curvature on the other side.

Statement (II): Concave lens always forms a virtual and erect image.

Now, considering the second statement, a concave lens (diverging lens) indeed always forms virtual, erect, and diminished images.

This is a fundamental property of concave lenses.

Given this analysis: The correct answer is Option A: Statement I is false but Statement II is true.

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