NCERT solutions for class 11 Physics chapter 15 Waves has been created by our team of subject experts with an objective to help students in their finals. These books include the solution for all the questions given in the NCERT Physics textbooks. By practicing questions from the NCERT solutions for class 11 Physics chapter 15, students can gain more information about the chapter and can also have a quick review before their finals.

This chapter comprises of comprehensive questions and solutions on a very important topic of physics such as questions on Waves dynamics etc. This has been asked repeatedly on exams and this chapter will guide you through every topics and types of waves such as tension on strings, speed of sound in air, transverse wave, dependence of speed of sound in air on factors like pressure, humidity and temperature. This chapter also has questions on concepts like wavelength of ultrasonic sound, transverse harmonic wave and their frequency etc.

Usually, in these problems we have taken a wire as a reference for signifying a wave motion and we have talked about transverse displacement of a wire which is clamped on both sides and in which, we will be talking about finding the amplitude of a point at a certain distance in the wire. We also have questions regarding calculating the speed of sound in a wire with pistons at the end and the other end is in resonance with a tuning fork. These topics are very important during competitive exams as well because waves being one of the important topic in physics, is being repeatedly asked in every sort of exam. You can check out NCERT Solutions for class 11 Physics for more chapterwise solutions.

We can know a lot about waves by solving questions on the speed of sound in a steel medium. There are questions on how your guitar strings produce sounds and what kind of frequency does each string of a guitar has. We have explanation on how a sound wave’s pressure antinode is a displacement node and vice versa also. We will be seeing how a dolphin being blind can maneuver through obstacles in a river and hunts preys. If a man is standing at a certain distance from an observer and he blows a horn, we can know what is the horn’s frequency if the man is running towards or away from the observer. Similar example can be found of a truck blowing horn at a man in a petrol pump, finding its frequency, speed and wavelength.

Waves characteristics comprises of its frequency, amplitude, wavelength, phase, resonance, displacement of waves such as longitudinal and transverse motion in various medium such as materials with high and low density, air, steel wires in guitars, sea waves etc.

**Q1. A 5 kg string is under 400 Newton of tension. The string is stretched to 40.0 m. If one end of the string is given a transverse jerk, find the amount of time taken by the disturbance take to reach the other end?**

Ans:

Given,

Mass of the string, M = 5 kg

Tension in the string, T = 400 N

Length of the string, l = 40.0 m

Mass per unit length, μ = M /l = 5/40 = 0.125 kg / m

We know,

Velocity of the transverse wave , v = \(\sqrt{\frac{T}{\mu }}\)

= \(\sqrt{\frac{400}{0.125 }}\) = 56.56 m/s

Therefore, time taken by the transverse wave to reach the other side, t = l/v = 40/56.56

= 0.707 s

**Q2.**** A shoe is dropped into a lake from a bridge that is 150 m above it. Given that the speed of sound in air is 340 m / s, find the amount of time taken by the sound of the shoe splashing the water to reach the top of the bridge? (g= 9.8 m s ^{-2})
**

**Ans:**

Given,

Height of the bridge, s = 150 m

Initial velocity of the shoe, u = 0

Acceleration, a = g = 9.8 m / s^{2}

Speed of sound in air = 340 m/s

Let t be the time taken by the shoe to hit the water’s surface

We know,

s = ut + ½ gt^{2}

150 = 0 + ½ x 9.8 x t^{2}

therefore, t^{2} = 300 / 9.8 = 5.53 s

Time taken by the sound to reach the bridge, t’= 150/340 = 0.44 s

Therefore from the moment the shoe is released from the bridge, the sound of it splashing the water is heard after = t +t’ = 5.53 + 0.44 = 5.97s

**Q3. A steel wire of mass 2 kg and length 24 m, allows a transverse wave to move through it at a speed equal to the speed of sound in dry air at 20 °C i.e., 343 m / s. Calculate the tension in the wire.**

**Ans:**

Given,

Length of the steel wire, l = 24 m

Mass of the steel wire, m = 2.0 kg

Velocity of the transverse wave, v = 343 m/s

Mass per unit length, μ = M /l = 2/24 = 0.083 kg / m

We know,

Velocity of the transverse wave , v = \(\sqrt{\frac{T}{\mu }}\)

Therefore, T = v^{2} μ

= 343^{2} x 0.083 = 9764.87 N

**Q4. Using the formula v = \(\sqrt{\frac{\gamma P}{\rho }}\) explain why the speed of sound in air
( a ) does not depend upon pressure.
( b ) increases with temperature and humidity.
( c ) increases with humidity.**

**Ans:**

Given,

v = \(\sqrt{\frac{\gamma P}{\rho }}\)

We know,

PV = nRT ( for n moles of ideal gas )

=> PV = RT (m/M )

Where, m is the total mass and M is molecular mass of the gas.

therefore, P = m (RT/M)

=> P = \(\frac{\rho RT}{M}\)

=> \(\frac{P}{\rho} = \frac{ RT}{M}\)

**( a )** For a gas at a constant temperature,\(\frac{P}{\rho}\)

= constant

Thus, as P increases ρ and vice versa. This means that P/ρ ratio always remains constant meaning

v =\(\sqrt{\frac{\gamma P}{\rho }}\)

= constant i.e., velocity of sound does not depend upon the pressure of the gas.

**( b )** Since, \(\frac{P}{\rho} = \frac{ RT}{M}\)

v = \(\sqrt{\frac{\gamma P}{\rho }}\) = v = \(\sqrt{\frac{\gamma RT}{M }}\)

We can see that v \(\propto \sqrt{T}\) i.e., speed of sound increases with temperature.

**( c )** When humidity increases, effective density of the air decrease. This means \(v \propto \frac{1}{\sqrt{\rho }}\), thus velocity increases.

**Q5.We know that the function y = f (x, t) represents a wave traveling in one direction, where x and t must appear in the combination x + vt or x– vt or i.e. y = f (x ± vt). Is the converse true?
Can the following functions for y possibly represent a travelling wave:
( i ) (x – vt) **

^{2}( ii ) log [ ( x + vt)/ x

_{0}] ( iii ) 1 / (x + vt )

Ans:

No, the converse is not true, because it is necessary for a wave function representing a traveling wave to have a finite value for all values of x and t.

As none of the above functions satisfy the above condition, thus, none represent a traveling wave.

**Q6. A flying-fox emitting ultrasonic sound at 1000 kHz is flying over a pond, when this sound meets the water surface, calculate the wavelength of ( i ) the reflected sound, ( ii ) the transmitted sound. [Speed of sound in air is 340 m / s and in water 1486 m / s]**

**Ans:**

Given,

Frequency of the ultrasonic sound, ν = 1000 kHz = 10^{6} Hz

Speed of sound in air, v_{A} = 340 m/s

We know,

( i ) The wavelength ( λ_{R} ) of the reflected sound is :

λ_{R} = v_{A} /v

= 340/10^{6} = 3.4 x 10^{-4 }m

( ii ) Speed of sound in water, v_{W} = 1486 m/s

Therefore, the wavelength (λ_{T })of the transmitted sound is :

λ_{T} = 1486 / 10^{6}

= 1.49 x 10^{-3} m

**Q7. An ultrasonic scanner operating at 4.2 MHz is used to locate tumors in tissues. If the speed of sound is 2 km /s in a certain tissue, calculate the wavelength of sound in this tissue?**

**Ans:**

Given,

Speed of sound in the tissue, v_{T} = 2 km/s = 2 × 10^{3} m/s

Operating frequency of the scanner, ν = 4.2 MHz = 4.2 × 10^{6} Hz

Therefore, the wavelength of sound:

λ = v_{T} / v

= (2 × 10^{3})/ (4.2 × 10^{6})

= 4.76 x 10^{-4} m

**Q8. A transverse harmonic wave on a wire is expressed as:
y( x, t ) =3 sin ( 36t +0.018x +**

**π**

**/**

**4**

**)**

( i ) Is it a stationary wave or a travelling?

( ii ) If it is a travelling wave, give the speed and direction of its propagation.

( iii ) Find its frequency and amplitude.

( iv ) Give the initial phase at the origin.

( v ) Calculate the smallest distance between two adjacent crests in the wave?

[X and y are in cm and t in seconds. Assume the left to right direction as the positive direction of x]

( i ) Is it a stationary wave or a travelling?

( ii ) If it is a travelling wave, give the speed and direction of its propagation.

( iii ) Find its frequency and amplitude.

( iv ) Give the initial phase at the origin.

( v ) Calculate the smallest distance between two adjacent crests in the wave?

[X and y are in cm and t in seconds. Assume the left to right direction as the positive direction of x]

**Ans:**

Given,

y(x, t) =3 sin (36t +0.018x + π/4) . . . . . . . . . . . ( 1 )

( i ) We know, the equation of a progressive wave travelling from right to left is:

y (x, t) = a sin (ωt + kx + Φ) . . . . . . . . . . . . . . . . . . . ( 2 )

Comparing equation ( 1 ) to equation ( 2 ), we see that it represents a wave travelling from right to left and also we get:

a = 3 cm, ω = 36 rad/s , k = 0.018 cm and ϕ = π/4

( ii )Therefore the speed of propagation , v = ω/k = 36/ 0.018 = 20 m/s

( iii ) Amplitude of the wave, a = 3 cm

Frequency of the wave v = ω / 2π

= 36 /2π = 5.7 hz

( iv ) Initial phase at the origin = π/4

( v ) the smallest distance between two adjacent crests in the wave, λ = 2π/ k = 2π / 0.018

= 349 cm

**Q9. For the wave in the above question (Q8), plot the displacement (y) versus (t) graphs for x = 0, 2 and 4 cm. ( i ) Give the shapes of these plots.
( ii ) With respect to which aspects (amplitude, frequency or phase) does the oscillatory motion in a travelling wave differ from one point to another?**

**Ans:**

Given,

y(x, t) =3 sin (36t +0.018x + π/4) . . . . . . . . . . . ( 1 )

For x= 0, the equation becomes :

y( 0, t ) =3 sin ( 36t +0 + π/4 ) . . . . . . . . . . . ( 2 )

Also,

ω = 2 π/t = 36 rad/s

=> t = π/18 secs.

Plotting the displacement (y) vs. (t) graphs using different values of t listed below:

t | 0 | T/ 8 | 2T/ 8 | 3T/ 8 | 4T/ 8 | 5T/ 8 | 6T/ 8 | 7T/ 8 | T |

y | \(\frac{3}{\sqrt{2}}\) | 3 | \(\frac{3}{\sqrt{2}}\) | 0 | \(\frac{-3}{\sqrt{2}}\) | -3 | \(\frac{-3}{\sqrt{2}}\) | 0 | \(\frac{3}{\sqrt{2}}\) |

Similarly graphs are obtained for x = 0, x = 2 cm, and x = 4 cm. The oscillatory motion in the travelling wave is different from each other only in terms of phase. Amplitude and frequency are invariant for any change in x.

The y-t plots of the three waves are shown in the given figure:

** Q10. A travelling harmonic wave is given as: y (x, t) = 2.0 cos 2π (10t – 0.0080x + 0.35).
What is the phase difference between the oscillatory motion of two points separated by a distance of:
( i ) 8 m,
( ii ) 1 m,
( iii ) λ /2,
( iv ) 6λ/4
[ X and y are in cm and t is in secs ].**

**Ans:**

Given,

Equation for a travelling harmonic wave :

y (x, t) = 2.0 cos 2π (10t – 0.0080x + 0.35)

= 2.0 cos (20πt – 0.016πx + 0.70 π)

Where,

Propagation constant, k = 0.0160 π

Amplitude, a = 2 cm

Angular frequency, ω= 20 π rad/s

We know,

Phase difference Φ = kx = 2π/ λ

( i ) For x = 8 m = 800 cm

Φ = 0.016 π × 800 = 12.8 π rad

( ii )For x = 1 m = 100 cm

Φ = 0.016 π × 100 = 1.6 π rad

( iii ) For x =λ /2

Φ = (2π/ λ) x ( λ/2)

= π rad

( iv ) For x =λ6 /4

Φ = (2π/ λ) x ( 6λ/4)

= 3 π rad

**Q11. The transverse displacement of a wire (clamped at both its ends) is described as :
y (x, t) = \(0.06sin(\frac{2\pi}{3}x)cos(120\pi t)\)
The mass of the wire is 6 x 10**

^{-2}kg and its length is 3m. Provide answers to the following questions: ( I ) Is the function describing a stationary wave or a travelling wave? ( ii ) Interpret the wave as a superposition of two waves travelling in opposite directions. Find the speed, wavelength and frequency of each wave. ( iii ) Calculate the wire’s tension. [X and y are in meters and t in secs]

**Ans:**

We know,

The standard equation of a stationary wave is described as:

y (x, t) = 2a sin kx cos ωt

Our given equation y (x, t) =\(0.06sin(\frac{2\pi}{3}x)cos(120\pi t)\) is similar to the general equation .

( i ) Thus, the given function describes a stationary wave.

( ii ) We know, a wave travelling in the positive x – direction can be represented as :

y_{1} = a sin( ωt – kx )

Also,

Wave travelling in the negative x – direction is represented as :

y_{2} = a sin( ωt + kx )

Super- positioning these two waves gives us :

y = y_{1} + y_{2}

= a sin( ωt – kx ) – a sin( ωt + kx )

= asin(ωt)cos(kx) – asin(kx)cos(ωt) – asin(ωt)cos(kx) – asin(kx)cos(ωt)

= – 2asin(kx)cos(ωt)

= \(-2asin(\frac{2\pi }{\lambda }x)cos(2\pi vt)\) . . . . . . . . . . . . . . ( 1 )

The transverse displacement of the wires is described as :

\(0.06sin(\frac{2\pi}{3}x)cos(120\pi t)\) . . . . . . . . . . . . . . . . .( 2 )

Comparing equations ( 1 ) and ( 2 ) , we get :

2π/ λ = 2π/ 3

Therefore, wavelength λ = 3m

Also, 2πv/λ = 120π

Therefore, speed v = 180 m/s

And, Frequency = v/λ = 180/3

= 60 Hz

( iii )Given,

Velocity of the transverse wave, v = 180 m / s

The string’s mass, m = 6 × 10^{-2} kg

String length, l = 3 m

Mass per unit length of the string, μ = m/l = (6 x 10^{-2 })/3

= 2 x 10^{-2} kg/m

Let the tension in the wire be T

Therefore, T = v^{2} μ

= 180^{2} x 2 x 10^{-2}

= 648 N.

Q12. Considering the wave described in the above question ( Q11 ) answer the following questions;

( a ) Are all the points in the wire oscillating at the same values of (i) frequency, (ii) phase, (iii) amplitude? Justify your answers.

( b ) Calculate the amplitude of a point 0.4 m away from one end?

**Ans:**

**( a )** As the wire is clamped at both its ends, the ends behave as nodes and the whole wire vibrates in one segment. Thus,

( i ) Except at the ends which have zero frequency, all the particles in the wire oscillate with the same frequency.

( ii ) All the particles in the wire lie in one segment, thus they all have the same phase. Except for the nodes.

( iii ) Amplitude, however, is different for different points.

**( b )** Given equation,

y (x, t) =\(0.06sin(\frac{2\pi}{3}x)cos(120\pi t)\)

For x = 0.4m and t =0

Amplitude = displacement =\(0.06sin(\frac{2\pi}{3}x)cos0 \)

= \(0.06sin(\frac{2\pi}{3}\times 0.4)1\)

= 0.044 m

**Q13. Present below are functions of x and t to describe the displacement (longitudinal or transverse) of an elastic wave. Identify the ones describing ( a ) a stationary wave, ( b ) a traveling wave and ( c ) neither of the two :
( i ) y = 3 sin( 5x – 0.5t ) + 4cos( 5x – 0.5t )
( ii ) y = cosxsint + cos2xsin2t.
( iii ) y = 2 cos (3x) sin (10t)
( iv ) y = \(2\sqrt{x – vt}\)**

**Ans:**

**( i )** This equation describes a traveling wave as the harmonic terms ωt and kx are in the combination of kx – ωt.

**( ii )** This equation describes a stationary wave because the harmonic terms ωt and kx appear separately in the equation. In fact, this equation describes the superposition of two stationary waves.

**( iii )** This equation describes a stationary wave because the harmonic terms ωt and kx appear separately.

**( iv )** This equation does not contain any harmonic term. Thus, it is neither a traveling wave nor a stationary wave.

**Q14. A string clamped at both its ends is stretched out, it is then made to vibrate in its fundamental mode at a frequency of 45 Hz. The linear mass density of the string is 4.0 × 10 ^{-2} kg/ m and its mass is 2 × 10 ^{-2} kg. Calculate:**

( i ) the velocity of a transverse wave on the string,

( ii ) the tension in the string.

**Ans:**

Given,

Mass of the string, m = 2 x 10^{-2} kg

Linear density of the string = 4 x 10^{-2} kg

Frequency, v_{F} = 45 Hz

We know, length of the wire = m/µ

= (2 x 10^{-2})/ (4 x10^{-2}) = 0.5 m

We know, λ = 2l/n

Where, n = number of nodes in the wire.

For fundamental node, n =1

=> λ = 2l

= 2 x 0.5 = 1m

( i ) Therefore speed of the transverse wave, v = λ v_{F}

= 1 x 45 = 45 m/s

( ii ) Tension in the string = µ v^{2}

= 4 x10^{-2} x 45 = 81 N

Q15. A 1m long pipe with a movable piston at one end and an opening at the other will be in resonance with a tuning fork vibrating at 340 Hz, if the length of the pipe is 79.3 cm or 25.5 cm. Calculate the speed of sound in air. Neglect the edge effects.

**Ans:**

Given,

Frequency of the turning fork, ν_{F} = 340 Hz

Length of the pipe, l_{1} = 0.255 m

As the given pipe is has a piston at one end, it will behave as a pipe with one end closed and the other end open, as depicted in the figure below:

This kind of system creates odd harmonics. We know, fundamental note in a closed pipe is written as:

l_{1} = λ / 4

0.255 x 4 = λ = 1.02m

Therefore speed of sound, v = λ v_{F
}= 340 × 1.02 = 346.8 m/s

**Q16. A steel bar of length 200 cm is nailed at its mid – point. The fundamental frequency of longitudinal vibrations of the rod is 2.53 kHz. At what speed will the sound be able to travel through steel?**

**Ans:**

Given,

Length , l = 200 cm = 2 m

Fundamental frequency of vibration, ν_{F} = 2.53 kHz = 2.53 × 10^{3} Hz

The bar is then plucked at its mid – point, forming an antinode (A) at its center, and nodes (N) at its two edges, as depicted in the figure below :

The distance between two successive nodes is λ / 2

=> l = λ / 2

Or, λ = 2 x 2 = 4m

Thus, sound travels through steel at a speed of v = νλ

v = 4 x 2.53 x 10^{3}

=10.12 km / s

Q17. One end of A 20 cm long tube is closed. Find the harmonic mode of the tube that will be resonantly excited by a source of frequency 430 Hz. lf both the ends are open, can the same source still produce resonance in the tube? (Sound travels in air at 340 m /s).

**Ans:**

Given,

Length of the pipe, l = 20 cm = 0.2 m

Frequency of the source = n^{th}

the normal mode of frequency, ν_{N} = 430 Hz

Speed of sound, v = 340 ms ^{-1}

We know, that in a closed pipe the n^{th} normal mode of frequency v_{N }^{ }= ( 2n -1 )v/4l

where n is an integer = 0, 1, 2, 3, 4, . . . . .

430 = ( 2n – 1 )( 340/4 x0.2)

2n = 2.01

n ≈ 1

Thus, the given source resonantly excites the first mode of vibration frequency

Now, for a pipe open at both the ends, the n^{th} mode of vibration frequency:

V_{R} = nv/2l

n = V_{R} 2l/v

n = (2 x 0.2 x 430)/340 = 0.5

As the mode of vibration ( n ) has to be an integer, this source is not in resonance with the tube.

Q18. Guitar strings X and Y striking the note ‘Ga’ are a little out of tune and give beats at 6 Hz. When the string X is slightly loosened and the beat frequency becomes 3 Hz. Given that the original frequency of X is 324 Hz, find the frequency of Y.

**Ans:**

Given,

Frequency of X, f_{X} = 324 Hz

Frequency of Y = f_{Y}

Beat’s frequency, n = 6 Hz

Also,

n = \(\left | f_{X}+f_{Y} \right |\)

6 = \(324 \pm f_{Y}\)

=> f_{Y} = 330 Hz or 318 Hz

As frequency drops with decrease in tension in the string, thus f_{Y} cannot be 330 Hz

=> f_{Y} = 318 Hz

Q19. Explain how:

( i ) A sound wave’s pressure antinode is a displacement node and vice versa.

( ii ) The Ganges river dolphin despite being blind, can maneuver and swim around obstacles and hunt down preys.

( iii ) A guitar note and violin note are being played at the same frequency, however, we can still make out which instrument is producing which note

( iv ) Both transverse and longitudinal wave can propagate through solids, but only longitudinal waves can move through gases.

( v ) In a dispersive medium, the shape of a pulse propagating through it gets distorted.

**Ans:**

** ( i )** An antinode is a point where pressure is the minimum and the amplitude of vibration is the maximum. On the other hand, a node is a point where pressure is the maximum and the amplitude of vibration is the minimum.

**( ii )** The Ganges river dolphin sends out click noises which return back as vibration informing the dolphin about the location and distances of objects in front of it. Thus, allowing it to maneuver and hunt down preys with minimum vision.

**( iii )** The guitar and the violin produce overtones of different strengths. Thus, one can differentiate between the notes coming from a guitar and a violin even if they are vibrating at the same frequencies.

**( iv )** Both solids and fluids have a bulk modulus of elasticity. Thus, they both allow longitudinal waves to propagate through them. However, unlike solids, gases do not have shear modulus. Thus, transverse waves cannot pass through gases.

**( v )** A pulse is a combination of waves of un-similar wavelengths. These waves move at different velocities in a dispersive medium. This causes the distortion in its shape.

**Q20. A man standing at a certain distance from an observer blows a horn of frequency 200 Hz in still air. ( a ) Find the horn’s frequency for the observer when the man ( i ) runs towards him at 20 m/s ( ii ) runs away from him at 20 m /s.
( b ) Find the speed of sound in both the cases.
[Speed of sound in still air is 340 m/ s]**

**Ans:**

Given,

Frequency of the horn, ν_{H} = 200 Hz

Velocity of the man, v_{T }= 20 m/ s

Velocity of sound, v = 340 m/ s

**( a )** We know,

(i) The apparent frequency of the horn as the man approaches the observer is:

v’ = v_{H }[ v/(v – v_{T}) ]

= 200 [ 340 /(340 – 20) ]

= 212.5 Hz

(ii) The apparent frequency of the horn as the man runs away from the observer is:

v’’ = v_{H }[ v/(v + v_{T}) ]

= 200 [ 340 /(340 + 20) ]

= 188.88 Hz

**( b )** The speed of sound is 340 m/s in both the cases. The apparent change in frequency is a result of the relative motions of the observer and the source.

**Q21. A truck parked outside a petrol pump blows a horn of frequency 200 Hz in still air. The Wind then starts blowing towards the petrol pump at 20 m /s. Calculate the wavelength, speed, and frequency of the horn’s sound for a man standing at the petrol pump. Is this situation completely identical to a situation when the observer moves towards the truck at 20 m /sand the air is still?
**

**Ans:**

For the standing observer:

Frequency, ν_{H} = 200 Hz

Velocity of sound, v = 340 m/s

Speed of the wind, v_{W} = 20 m/s

The observer will hear the horn at 200 Hz itself because there is no relative motion between the observer and the truck.

Given that the wind blows in the observer’s direction at 20 m/s.

Effective velocity of the sound, v_{E} = 340 + 20 = 360 m/s

The wavelength ( λ ) of the sound :

λ = v_{E }/v_{H } = 360/200

λ = 1.8 m

For the observer running towards the train :

Speed of the observer, v_{o} = 20 m/s

We know,

The apparent frequency of the sound as the observers moves towards the truck is :

v’ = v_{H} [(v + v_{o})/v ]

= 200[ (20 + 340 )/ 340 ] = 211.764 Hz

As the air is still the effective velocity of sound is still 340 m/s.

As the truck is stationary the wavelength remains 1.8 m.

Thus, the two cases are not completely identical.