Class 9 Science Chapter 10 Sound Waves NCERT Solutions | Boundless Maths
📗 Exploration · CBSE 2026-27 Unit III · Motion, Force & Sound ✨ Free — No Sign-up 62 Questions

Class 9 Science Chapter 10:
Sound Waves: Characteristics and Applications

Class 9 Science Chapter 10, Sound Waves: NCERT question answers for every Think It Over, Activity, Pause & Ponder, Worked Example, What If, Revise Reflect Refine and Journey Beyond question (CBSE 2026-27), with full working for every numerical. Keep your Class 9 Science chapter 10 notes handy and check each answer here.

Sound Waves asks how vibrations become something we can hear, and these Class 9 Science Chapter 10 NCERT solutions cover how sound travels as compressions and rarefactions, the wave equation v = λν numericals, the difference between loudness and pitch, echo distance and SONAR depth problems, and the uses of ultrasonic and infrasonic waves, with every numerical worked step by step.

Last updated 20 October 2026 · Reviewed by Suchita Arora, 13+ years teaching CBSE Maths & Science

62
Questions Solved
9
Question Sections
₹0
Cost — Always Free
100%
In-text Coverage
Overview

What Chapter 10 Is Really About

Sound Waves: Characteristics and Applications takes sound from something you simply hear to something you can measure. It builds up how sound is produced by vibrations, why it needs a medium to travel as a longitudinal mechanical wave of compressions and rarefactions, and how that wave is described using wavelength, frequency, time period, amplitude and speed, connected by v = λν. It closes with echo and reverberation, and how ultrasonic and infrasonic waves power SONAR, echolocation and medical imaging. Every question is solved here, section by section, as complete Class 9 Science Chapter 10 NCERT solutions with answers.

🌊

Production & Propagation

Vibration as the source of every sound, why a medium (solid, liquid or gas) is essential, and how compressions and rarefactions form a longitudinal wave.

📊

Wave Characteristics

Wavelength, frequency, time period, amplitude and speed — and the one equation, v = λν, that ties every numerical in this chapter together.

🦇

Reflection & Applications

Echo, reverberation, pitch and loudness, plus ultrasonic and infrasonic waves behind SONAR, echolocation and medical ultrasound.

Section A

Think It Over (Chapter Opener)

2 Questions
Q1Two astronauts are repairing the arm of a space station together during a spacewalk. Can they talk to each other and hear the sounds of metal clanking as they do on the Earth?▾

Sound is a mechanical wave and needs a material medium (solid, liquid or gas) to travel.

Outer space is a near vacuum, so there is no medium between the astronauts.

So the sound of their voices or of the metal clanking cannot travel from one astronaut to the other.

They talk to each other through special communication devices (radio) fitted in their spacesuits. Radio waves do not need a medium.

Answer
No. They cannot talk directly or hear the clanking, because sound cannot travel through a vacuum. They use radio devices in their suits.
Q2How do most bats use sound to locate their prey in the dark at night?▾

A bat sends out short bursts of ultrasonic waves (frequency above 20 kHz).

These waves strike the prey or obstacles and get reflected back as echoes.

The bat senses the echoes. The time taken by the echo and its direction tell the bat the position of the prey or obstacle.

This method of locating objects using reflected sound is called echolocation.

Answer
Bats emit ultrasonic waves and detect the echoes reflected from the prey. This is called echolocation.
Section B

Activities 10.1 – 10.8

8 Questions
10.1Activity 10.1: Let us explore1.Take a cardboard box with one side open and a rubber band.2.Stretch the rubber band across the open side of the box (Fig. 10.2).3.Holding the box steady with one hand, pluck the rubber band with a finger. Do you hear any sound?4.Pluck the rubber band again and watch it carefully. Is it vibrating?5.Wait till the rubber band stops vibrating. Do you still hear the sound?6.Change the tension in the rubber band by stretching it more or loosening it slightly and plucking it each time. Does the sound change? What changes do you notice?7.Remove the rubber band from the box. Stretch it between two fingers and pluck it near your ear. Is the sound still produced? Is it as loud as before?▾
A cardboard box open on one side with a rubber band stretched across it
Fig. 10.2 — Rubber band across a box

Step 3: Yes, a sound is heard.

Step 4: Yes, the rubber band is seen vibrating (moving to and fro rapidly).

Step 5: No. When the vibration stops, the sound also stops.

Step 6: Yes, the sound changes. A more stretched (tighter) band vibrates faster and gives a higher pitch (shriller sound). A loosened band vibrates slower and gives a lower pitch.

Step 7: Yes, sound is still produced, but it is fainter, not as loud as before. The box is not there to strengthen the sound.

Conclusion
Sound is produced by vibrations. As long as the object vibrates, sound is produced, and when the vibration stops, the sound stops.
10.2Activity 10.2: Let us explore1.Take a tuning fork and a soft rubber pad.2.Hold the tuning fork by its stem.3.Strike one of the prongs of the tuning fork gently against the rubber pad (Fig. 10.4b) and bring it close to your ear. Do you hear a sound? (Take care not to strike the tuning fork against a hard surface).4.Now, gently touch a water surface with one of the vibrating prongs of the tuning fork. Do you see waves forming on the surface of water?5.Repeat step 3 a few times while bringing the prongs of the tuning fork near your ear in different orientations. Do you hear the sound?▾
A tuning fork showing its prongs and stem beside a black rubber pad
(a) Tuning fork and rubber pad
A hand striking a prong of a tuning fork against a rubber pad
(b) Striking against the pad
A vibrating prong of a tuning fork dipped in water making ripples
(c) Prong in water
Fig. 10.4 — Activity 10.2 with a tuning fork

Step 3: Yes, a clear sound is heard from the vibrating tuning fork.

Step 4: Yes, the vibrating prong makes waves and splashes in the water.

Step 5: Yes, the sound is heard in every orientation. This shows that sound spreads in all directions from the source.

Conclusion
The prongs of a sounding tuning fork are vibrating. This supports the idea that sound is produced by vibrating objects.
10.3Activity 10.3: Let us investigate1.You and your friend stand on opposite sides of a desk in the classroom. Let your friend gently knock or scratch on the desk. Listen carefully to the sound produced with your ear in the air.2.Now, place your ear against the desk, close your other ear and listen again, as shown in Fig. 10.5. Are you able to hear the sound through the table?▾
A girl and a boy on opposite sides of a desk; the boy rests his ear on the desk while the girl taps it
Fig. 10.5 — Investigating if sound travels through solid objects

Step 1: The sound is heard, but it is faint.

Step 2: Yes, the sound is heard and it is louder and clearer through the desk.

Conclusion
Sound can travel through solids, such as a wooden desk.
10.4Activity 10.4: Let us investigate1.Take a large tub or bucket of water filled to the brim and two metal spoons.2.Tap the spoons against one another and listen to the sound produced (Fig. 10.6a).3.Now, submerge the two metal spoons in water without touching the sides or bottom of the bucket and tap them against one another again (Fig. 10.6b). Do you again hear the sound produced?▾
Two spoons held above an empty glass tub
Spoons tapped in air
Two spoons tapped together under water in a glass tub
Spoons tapped under water
Fig. 10.6 — Tapping two spoons against each other

Step 2: A clear ringing sound is heard in air.

Step 3: Yes, the sound is heard again, though it may be a little different.

The sound has reached our ear after travelling through water and then air.

Conclusion
Sound can travel through liquids. Sound travels through solids, liquids and gases.
10.5Activity 10.5: Let us observe1.Take a slinky and a marker.2.Make a mark on a turn of the slinky with the marker. Lay out the slinky horizontally on a table or floor.3.Ask a friend to hold one end of the slinky fixed while you hold the other end keeping the slinky slightly stretched.4.Give the slinky at your end a sharp push towards your friend and then quickly pull it back again (Fig. 10.8). Do you observe a disturbance created in the slinky which moves towards your friend?5.Now, push and pull the slinky end multiple times in quick succession (The pulling and pushing of the end of the slinky is similar to the sound being produced continuously). Are a series of disturbances produced in the slinky? Do these disturbances move across the length of slinky? Does the mark on the slinky move back and forth parallel to the direction of the disturbance?▾
A slinky stretched between two hands, with a compressed part and a spread-out part travelling along it
Fig. 10.8 — Disturbance travelling along a slinky

Step 4: Yes. A region where the turns are closer together moves along the slinky towards the friend.

Step 5: Yes. A series of regions with closely spaced turns and regions with spread out turns is produced.

These regions move along the whole length of the slinky.

The mark does not travel along with the disturbance. It only moves back and forth about its own position, parallel to the direction in which the disturbance travels.

Conclusion
Sound travels in a similar way. The disturbance (compressions and rarefactions) travels through the medium, but the particles of the medium only vibrate about their mean positions.
10.6Activity 10.6: Let us experiment1.Take a wide mouthed container, a cellophane or rubber sheet (such as that of a balloon) of size larger than its opening, a loud sound source (such as a metal plate and a beater) and some grains or particles (such as rice, semolina, salt, or chalk powder).2.Stretch the sheet over the edges of the container tightly and fix it with tape or a rubber band (Fig. 10.14).3.Sprinkle the grains evenly over the sheet, ensuring they are not clumped together.4.Produce a loud sound near the bowl without touching it. Observe the grains on the sheet. Does the sound have any effect on the grains?5.Repeat step 4 with different sources of sounds and observe the effect on the grains. You can try increasing or reducing the volume of sound. Try with different grains.▾
Grains on a sheet over a bowl while a plate is struck above it
Fig. 10.14 — Sound moving grains (coloured)

Step 4: Yes. The grains move and jump on the sheet.

Step 5: A louder sound makes the grains jump higher, and a softer sound makes them move less. The effect is seen with all kinds of grains.

Reason: The sound travels through the air and reaches the sheet. It makes the sheet vibrate, and the vibration moves the grains.

Conclusion
Sound is a form of energy. The vibrating source transfers energy to the air, and the air transfers it to the sheet, even though the source does not touch the sheet.
10.7Activity 10.7: Let us experiment (demonstration activity)
This activity is recommended to be performed as a classroom group activity facilitated by the teacher.1.Use a mobile app, such as Phyphox that can identify frequencies of sounds. Use the ‘Audio Spectrum’ option that displays the frequency graphically or in hertz (Hz).2.Try to sing the musical notes ‘Sa, Re, Ga, Ma, Pa, Dha, Ni, Sa’ one after another, or use a music or tone generating app on another phone to produce those notes. Observe how the frequency changes as each note is produced.3.Record the approximate frequency values for each musical note.4.Compare the musical notes by taking the ratio of each frequency with respect to the ‘Sa’. Do you observe any pattern?5.If both voice and mobile-generated notes are used, compare their frequencies for the same musical notes.
▾

Sample readings (the exact values depend on the pitch chosen for Sa):

NoteFrequency (Hz)Ratio to Sa
Sa2401
Re2701.125
Ga3001.25
Ma3201.33
Pa3601.5
Dha4001.67
Ni4501.875
Sa (upper)4802

Step 2: The frequency is lowest for the first Sa and keeps increasing for Re, Ga, Ma, Pa, Dha and Ni.

Step 4: The ratios are fixed numbers, which do not depend on the pitch of Sa. The upper Sa has a frequency exactly double that of the lower Sa (ratio 2).

Step 5: The values for the voice are close to those of the app, but slightly different because a voice cannot hold an exact frequency.

Conclusion
Each musical note has its own frequency, and the frequency increases from Sa to the upper Sa. The upper Sa has twice the frequency of the lower Sa.
10.8Activity 10.8: Let us experiment (demonstration activity)
This activity is recommended to be performed as a classroom group activity facilitated by teacher.1.Open a mobile app that can generate sounds.2.Set the frequency to 100 Hz, tap ‘play’, and listen carefully.3.Increase the frequency in steps of 100 Hz up to 1000 Hz and describe how the sound changes.4.Next, set the frequency to 50 Hz. Reduce the frequency till about 20 Hz or the point where you cannot hear the sound anymore.
▾

Step 2: A low, deep sound is heard at 100 Hz.

Step 3: As the frequency increases, the sound becomes higher in pitch, from deep to sharp and shrill. The pitch rises with frequency.

Step 4: At 50 Hz the sound is very deep. Near 20 Hz it is hardly heard, and below about 20 Hz nothing can be heard.

Conclusion
A higher frequency gives a higher pitch. Humans can hear sound only from about 20 Hz to 20,000 Hz.
Section C

Pause and Ponder

13 Questions
P1Explore various ways of producing sound.▾

Sound is produced whenever an object vibrates. Some ways are:

Way of producing soundExample
Plucking a stretched stringSitar, guitar, rubber band
Striking an objectTabla, drum, bell, tuning fork
Blowing air in a hollow pipeBansuri (flute)
Vibrating vocal cordsTalking, singing
Rubbing body partsCrickets and grasshoppers rub wings or legs
Clapping handsHands striking each other
Answer
Sound can be produced by plucking strings, striking objects, blowing air through pipes, vibrating vocal cords and rubbing surfaces. In every case, something vibrates.
P2Make a list of different types of musical instruments and identify their vibrating parts which produce sound.▾

Musical instruments are grouped by the part that vibrates:

InstrumentVibrating part
Sitar, veena, guitar, tanpuraStretched strings
Tabla, mridangam, drumStretched membrane (drum head)
Bansuri (flute)Air column inside the pipe
HarmoniumMetal reeds
Bell, cymbalsMetal body
XylophoneWooden or metal bars
Answer
Stringed instruments have vibrating strings, drums have vibrating membranes, and wind instruments have vibrating air columns.
P3Assertion (A): We cannot hear the sound of a bell ringing in a closed jar after most of the air is pumped out.
Reason (R): Sound requires a medium to travel.
Choose the correct statement:
(i) Both A and R are true, but R is not the correct explanation of A.
(ii) Both A and R are true, and R is the correct explanation of A.
(iii) A is true, but R is false.
(iv) A is false, but R is true.
▾
An electric bell inside a bell jar joined to a vacuum pump and a power supply
Fig. 10.7 — Illustration of a vacuum bell jar

Assertion (A): True. As the air is pumped out, the sound becomes fainter, and in a near vacuum almost no sound is heard.

Reason (R): True. Sound is a mechanical wave and needs a medium to travel.

Since there is no air (medium) left, the sound cannot reach us. So R explains A.

Answer
Option (ii): Both A and R are true, and R is the correct explanation of A.
P4Assertion (A): Compressions and rarefactions move through the medium.
Reason (R): Individual particles of the medium continuously move forward with the wave.
Choose the correct statement:
(i) Both A and R are true, but R is not the correct explanation of A.
(ii) Both A and R are true, and R is the correct explanation of A.
(iii) A is true, but R is false.
(iv) A is false, but R is true.
▾
(a) Not oscillating – average density(b) Forward motion – a compression(c) Backward motion – a rarefaction(d) Oscillating – C and R alternateCRCCRCRCwww.boundlessmaths.com
Fig. 10.9 — Density of air in a tube with a piston

Assertion (A): True. The compressions and rarefactions travel through the medium.

Reason (R): False. The particles do not move forward with the wave. They only vibrate to and fro about their mean positions.

Answer
Option (iii): A is true, but R is false.
P5When sound travels from a tuning fork to your ear, which of the following actually reaches your ear?
(i) Air particles near the tuning fork
(ii) Energy carried by sound waves
(iii) The tuning fork material
(iv) A continuous stream of compressed air
▾

The particles of air only vibrate about their mean positions. They do not travel from the fork to the ear, so (i) and (iv) are wrong.

The material of the tuning fork stays with the fork, so (iii) is wrong.

What reaches the ear is the disturbance (compressions and rarefactions), which carries energy.

Answer
Option (ii): Energy carried by sound waves.
P6The variation of density of the medium for two sound waves is shown in Fig. 10.17 (a) and (b). Label compression and rarefaction by C and R on it. In the graph given in Fig. 10.17 (c) and (d), label the axes and draw the curves corresponding to Fig. 10.17 (a) and (b).▾

A region where the dots are crowded has a high density. It is a compression (C), and it matches a crest of the graph.

A region where the dots are spread out has a low density. It is a rarefaction (R), and it matches a trough of the graph.

On the graph, distance is on the x-axis and density is on the y-axis. The dashed line is the average density.

Wave (a): the dense and sparse regions are close together (shorter wavelength), so the curve (c) has more waves.

C C C R R Distance Density crest trough www.boundlessmaths.com
Fig. 10.17 (a) and its graph (c): C = compression, R = rarefaction. The dashed line is the average density

Wave (b): the dense and sparse regions are farther apart (longer wavelength), so the curve (d) has fewer waves.

C C R R Distance Density crest trough www.boundlessmaths.com
Fig. 10.17 (b) and its graph (d): C = compression, R = rarefaction
Answer
Crowded regions are compressions (crests) and spread-out regions are rarefactions (troughs). Distance is on the x-axis and density on the y-axis.
P7Conduct Activity 10.1 once again with a thick rubber band and then with a thin rubber band. Does the thin rubber band vibrate faster than the thick rubber band? If yes, how do the frequency and time period of the sound produced by the thin rubber band differ from that of the thick rubber band?▾

Observation: Yes, the thin rubber band vibrates faster than the thick rubber band.

The thin band makes more vibrations in one second. So its frequency is higher, and it gives a higher pitch (shriller sound).

Time period is the time for one vibration, T = 1/ν. A higher frequency means a shorter time period.

Rubber bandSpeed of vibrationFrequencyTime period
ThinFasterHigherShorter
ThickSlowerLowerLonger
Answer
The thin band has a higher frequency and a shorter time period than the thick band.
P8If the frequency of a sound wave produced by an oscillating piston of a long tube filled with air is 20 Hz, then how many oscillations does the piston complete per minute?▾

Given: frequency ν = 20 Hz

To find: number of oscillations in 1 minute

Frequency 20 Hz means 20 oscillations in every second.

1 minute = 60 s

\[\text{Oscillations} = 20 \times 60 = 1200\]
Answer
The piston completes 1200 oscillations per minute.
P9For the sound wave represented by the graph shown in Fig. 10.19, what is half of its wavelength?▾

Wavelength is the distance between two consecutive crests.

From the graph, the crests are at 0.75 cm and 3.75 cm.

\[\lambda = 3.75 - 0.75 = 3.0\text{ cm}\]

Also, one full wave starts at 0 and ends at 3.0 cm, so λ = 3.0 cm.

Half of the wavelength:

\[\dfrac{\lambda}{2} = \dfrac{3.0}{2} = 1.5\text{ cm}\]
0 1.5 3.0 4.5 6.0 Distance (cm) Density λ = 3.0 cm λ/2 www.boundlessmaths.com
Fig. 10.19 (redrawn): crest to crest = 3.0 cm, so λ = 3.0 cm and λ/2 = 1.5 cm
Answer
Half of the wavelength is 1.5 cm.
P10Table 10.1 shows the speed of sound in a few media at atmospheric pressure.
Table 10.1: Speed of sound in different media at 15 °C
StateSubstance/MediumApproximate speed
SolidSteel5000 m s⁻¹
LiquidWater1500 m s⁻¹
GasAir340 m s⁻¹
Compare the speeds in different media by finding the ratio of
(i) the speed of sound in water with respect to the speed in the air.
(ii) the speed of sound in steel with respect to the speed in the water.
▾

Given: steel = 5000 m/s, water = 1500 m/s, air = 340 m/s

(i)Speed in water : speed in air
\[\dfrac{1500}{340} = 4.41\]
Ans.About 4.4 (sound is about 4.4 times faster in water)
(ii)Speed in steel : speed in water
\[\dfrac{5000}{1500} = 3.33\]
Ans.About 3.3 (sound is about 3.3 times faster in steel)
P11Two friends are standing along a steel fence at a distance of 340 m from each other (Fig. 10.23). Gunjan places her ear over the fence and her friend knocks the fence with a metal object. Using the values of the speed of sound in steel and air given in Table 10.1, calculate the time difference between the sound that reached Gunjan through the air and the steel. Would it have been possible for her to distinguish between the two sounds? (The time interval between two sounds must be at least 0.1 s to be heard separately.)▾
Two people standing at the ends of a long steel fence; one knocks the fence while the other listens with her ear on it
Fig. 10.23 — Time difference between the sound reaching through air and steel

Given: distance = 340 m, speed in steel = 5000 m/s, speed in air = 340 m/s

To find: time difference between the two sounds

Time = distance / speed

Through air:

\[t_{air} = \dfrac{340}{340} = 1\text{ s}\]

Through steel:

\[t_{steel} = \dfrac{340}{5000} = 0.068\text{ s}\]

Time difference:

\[\Delta t = 1 - 0.068 = 0.932\text{ s}\]

0.932 s is more than 0.1 s.

Answer
The time difference is about 0.93 s. Yes, she can distinguish the two sounds, first the sound through steel and then the sound through air.
P12An experiment is being set up that requires echoes to arrive at least 0.2 s after the emission of sound. What minimum distance should a reflecting surface be placed at? Assume the speed of sound to be 343 m s⁻¹.▾

Given: time t = 0.2 s, speed v = 343 m/s

To find: minimum distance of the reflecting surface

The sound goes to the surface and comes back, so the total distance covered = 2d.

\[2d = v \times t = 343 \times 0.2 = 68.6\text{ m}\] \[d = \dfrac{68.6}{2} = 34.3\text{ m}\]
Answer
The reflecting surface should be at least 34.3 m away.
P13Sound travels much farther in water than light, and thus, is used for various underwater applications. A sonar signal sent to find the depth of ocean takes 4 s to return. What is the depth of the ocean at that location if the speed of sound in seawater is 1500 m s⁻¹?▾

Given: total time t = 4 s, speed v = 1500 m/s

To find: depth of the ocean

The signal goes down and comes back, so the time to reach the bottom = 4/2 = 2 s.

\[d = v \times t = 1500 \times 2 = 3000\text{ m}\]
Answer
The depth of the ocean is 3000 m (3 km).
Section D

Worked Examples 10.1 – 10.6

6 Questions
Ex 10.1Example 10.1: If there are 10 density oscillations in 2 seconds at a given position, then calculate the (i) frequency of sound wave, and (ii) its time period.▾

Given: number of oscillations = 10, time = 2 s

(i)Frequency

Frequency = number of oscillations / time taken

\[\nu = \dfrac{10}{2\text{ s}} = 5\text{ Hz}\]
Ans.5 Hz
(ii)Time period

Time for one oscillation:

\[T = \dfrac{2\text{ s}}{10} = 0.2\text{ s}\]
Ans.0.2 s
Ex 10.2Example 10.2: Human hearing roughly spans 20 Hz to 20 kHz. What are the corresponding wavelengths in air for these two frequencies? Use the speed of sound in air as 344 m s⁻¹.▾

Given: speed v = 344 m/s; frequencies 20 Hz and 20 kHz = 20000 Hz

Using v = λ × ν, the wavelength is λ = v / ν.

(i)For ν = 20 Hz
\[\lambda = \dfrac{344}{20} = 17.2\text{ m}\]
Ans.17.2 m
(ii)For ν = 20 kHz = 20000 Hz
\[\lambda = \dfrac{344}{20000} = 0.0172\text{ m}\] \[= 1.72\text{ cm}\]
Ans.0.0172 m = 1.72 cm
Ex 10.3Example 10.3: During a thunderstorm, lightning is seen before thunder is heard because sound travels much slower than light. If the time delay between seeing the lightning flash and hearing the thunder is measured to be 5 s, estimate the distance to the lightning strike. Use the speed of sound in air as 340 m s⁻¹. Assume that light (speed = 300000 km s⁻¹) reaches you almost instantaneously.▾

Given: time delay t = 5 s, speed of sound v = 340 m/s

To find: distance to the lightning strike

Light reaches us almost at once, so the delay is the time taken by sound.

\[d = v \times t = 340 \times 5 = 1700\text{ m}\]
Answer
The lightning struck about 1700 m (1.7 km) away.
Ex 10.4Example 10.4: From the graphical representation of a sound wave propagating in steel (Fig. 10.22), find its wavelength. Calculate its frequency and time period if the speed of sound in steel is 5000 m s⁻¹.▾

Given: speed v = 5000 m/s

Wavelength: from the graph, the distance between two consecutive crests is 50 m.

0 25 50 75 100 Distance (m) Density λ = 50 m www.boundlessmaths.com
Fig. 10.22 (redrawn): the distance between two consecutive crests is 50 m
\[\lambda = 50\text{ m}\]

Frequency: using v = λ × ν

\[\nu = \dfrac{v}{\lambda} = \dfrac{5000}{50} = 100\text{ Hz}\]

Time period:

\[T = \dfrac{1}{\nu} = \dfrac{1}{100} = 0.01\text{ s}\]
Answer
Wavelength = 50 m, frequency = 100 Hz and time period = 0.01 s.
Ex 10.5Example 10.5: You clap in an empty corridor and hear an echo after 0.5 s. If the speed of sound in air is 340 m s⁻¹, calculate your distance from the wall.▾

Given: time t = 0.5 s, speed v = 340 m/s

To find: distance from the wall

The sound goes to the wall and comes back, so the total distance = 2d.

\[d = \dfrac{v \times t}{2} = \dfrac{340 \times 0.5}{2} = 85\text{ m}\]
Answer
The wall is 85 m away.
Ex 10.6Example 10.6: A naval sonar signal sent into seawater returns after 0.90 s. The speed of sound in seawater is 1530 m s⁻¹. How far is the object?▾

Given: total time = 0.90 s, speed v = 1530 m/s

To find: distance of the object

Time taken to reach the object = half of the total time:

\[t = \dfrac{0.90}{2} = 0.45\text{ s}\]

Distance:

\[d = v \times t = 1530 \times 0.45 = 688.5\text{ m}\]
Answer
The object is 688.5 m away.
Section E

What If...?

2 Questions
WI 1What if ...
the speed of sound in air depended on its frequency? Would music still sound pleasant when a singer performs with instruments? Why or why not?
▾

A musical note is a mixture of a fundamental frequency and higher frequencies (overtones). All of them leave the source together.

If the speed depended on frequency, the different frequencies would travel at different speeds and reach the listener at different times.

The sound would be blurred, especially for listeners sitting far from the stage. The notes of the singer and the instruments would also not stay in step.

Answer
No. The music would sound garbled and unpleasant, because the different frequencies would reach the listener at different times.
WI 2What if ...
humans could detect ultrasonic waves like dogs can? What would be the advantages and disadvantages?
▾

Advantages:

We could detect ultrasonic sounds from machines and find faults early. We could sense the high-pitched calls of animals, and use sound to find objects in the dark, like bats do.

Disadvantages:

We would hear a lot of extra sound from machines, electronic devices and animals all the time. This would cause noise, disturb sleep and concentration, and could harm hearing.

Answer
It would give us new abilities, such as sensing in the dark, but the constant extra noise would be distracting and could damage hearing.
Section F

Questions from the Text

4 Questions
IN1Which form of energy gets converted to sound energy? How is sound produced and how does it reach our ears?▾

Energy: The mechanical (kinetic) energy of a vibrating object is converted into sound energy. For example, the muscular energy of a person plucking a string or striking a drum.

Production: Sound is produced by vibrating objects, such as strings, membranes, air columns and vocal cords.

Reaching the ear: The vibrating source makes the particles of the medium (air) vibrate, which produces compressions and rarefactions. This disturbance travels through the medium and reaches the ear, where it makes the eardrum vibrate.

Answer
Mechanical energy is changed into sound energy. Vibrations of the source travel through a medium as compressions and rarefactions and reach our ears.
IN2Would you hear sound in vacuum?▾

A vacuum has no matter (no medium), so there are no particles to carry the vibrations.

In the bell jar experiment, the sound becomes fainter as air is pumped out, and almost no sound is heard in a near vacuum, though the bell is seen ringing.

Answer
No. Sound cannot propagate in a vacuum, because it needs a medium.
IN3If sound did not travel through liquids, would you have heard this sound?
(In Activity 10.4, two metal spoons are tapped against each other under water.)
▾

The spoons are inside the water, so the sound first travels through the water and then through the air to reach our ears.

We do hear the sound when the spoons are submerged. If liquids could not carry sound, no sound would have come out of the water.

Answer
No, we would not have heard it. We hear the sound, so sound does travel through liquids.
IN4If there is no medium (i.e., no particles), is the propagation of sound waves possible?▾

Sound waves are mechanical waves. They travel by the vibration of the particles of a medium and their collisions with the neighbouring particles.

Without particles, there is nothing to vibrate and pass on the disturbance.

Answer
No. Sound waves cannot propagate without a material medium.
Section G

Revise, Reflect, Refine

15 Questions
Q1Which observation best supports the idea that sound is a mechanical wave?
(i) Sound shows reflection
(ii) Sound needs a medium to propagate
(iii) Sound has frequency
(iv) Sound carries energy
▾

A mechanical wave is a wave that needs a material medium to propagate.

Reflection, frequency and carrying energy are properties of all waves, including light, which is not a mechanical wave.

Only the need for a medium shows that sound is a mechanical wave.

Answer
Option (ii): Sound needs a medium to propagate.
Q2For a sound wave propagating in a medium, increasing its frequency will increase its
(i) wavelength
(ii) speed
(iii) number of compressions per second
(iv) time period
▾

Speed depends only on the medium, so it stays the same. (ii) is wrong.

Since v = λν, with a fixed speed, a larger frequency gives a smaller wavelength. (i) is wrong.

Time period T = 1/ν decreases. (iv) is wrong.

Frequency is the number of oscillations (compressions) passing a point per second, so it increases.

Answer
Option (iii): number of compressions per second.
Q3If 20 compressions pass a point in 4 seconds, the frequency is
(i) 80 Hz
(ii) 5 Hz
(iii) 10 Hz
(iv) 0.2 Hz
▾

Given: 20 compressions (20 oscillations) in 4 s

Each compression passing means one oscillation.

\[\nu = \dfrac{20}{4\text{ s}} = 5\text{ Hz}\]
Answer
Option (ii): 5 Hz.
Q4In a room, the reflected sound reaches the ear 0.05 s after its production. Will it produce an echo or reverberation? Justify your answer.▾

An echo is heard only when the reflected sound arrives at least 0.1 s after the original sound.

Here the time gap = 0.05 s, which is less than 0.1 s, so the ear cannot hear the reflected sound separately.

Instead, the multiple reflections from the walls of the room blend with the original sound and make it persist. This is reverberation.

Answer
It will produce reverberation, not an echo, because the time gap (0.05 s) is less than 0.1 s.
Q5Graphs representing two sound waves are given in Fig. 10.30. If the scales on the X and Y axes of the two graphs are the same, which of the two sound waves has (i) greater wavelength, and (ii) smaller amplitude?▾

Wavelength is the distance between two consecutive crests. Amplitude is the maximum height of the curve above the average density line.

In the same length of the x-axis, wave (a) has 3 waves and wave (b) has 6 waves.

The curve of (a) rises and falls less from the average line than that of (b).

0 Distance Density www.boundlessmaths.com
(a) 3 waves, small height
0 Distance Density www.boundlessmaths.com
(b) 6 waves, large height
(i)Greater wavelength

Fewer waves in the same distance means longer waves.

Ans.Wave (a)
(ii)Smaller amplitude

Wave (a) has a smaller height above the average line.

Ans.Wave (a)
Q6The sound waves emitted by three sources A, B and C are represented in Fig. 10.31. If the frequency of A is maximum and C is minimum, identify the corresponding curves, and mark A, B and C on them.▾

Frequency is the number of waves per unit distance (or time). More waves in the same length means a higher frequency (a shorter wavelength).

The green curve has the most waves, the red curve has fewer, and the blue curve has the fewest.

CurveNumber of wavesFrequencySource
GreenMostMaximumA
RedIn betweenIn betweenB
BlueFewestMinimumC
0 Distance Density A B C www.boundlessmaths.com
Fig. 10.31 (redrawn): green has the most waves (A), red is in the middle (B), blue has the fewest (C)
Answer
Green is A, red is B and blue is C.
Q7Draw a graph to represent a sound wave for which the density amplitude is 3 units and wavelength is 4 cm.▾

Amplitude = 3 units, so the density rises 3 units above the average and falls 3 units below it.

Wavelength = 4 cm, so the crests are 4 cm apart.

Take distance (cm) on the x-axis and the change in density from the average on the y-axis.

Crests are at 1 cm and 5 cm (height +3), troughs are at 3 cm and 7 cm (height −3), and the curve crosses the average line at 0, 2, 4, 6 and 8 cm.

0 2 4 6 8 −3 0 +3 Distance (cm) Change in density λ = 4 cm amplitude = 3 www.boundlessmaths.com
Required graph: amplitude = 3 units, wavelength = 4 cm (two complete waves are drawn)
Answer
The graph is a wave with crests at +3 units and troughs at −3 units, and a distance of 4 cm between consecutive crests.
Q8In a movie, while showing the explosion of a spacecraft in space, a flash of light is shown along with sound at the same time. What are the errors in this depiction?▾

Error 1: Space is a near vacuum. Sound cannot travel without a medium, so no explosion sound can be heard.

Error 2: Light travels much faster than sound (300000 km/s compared with about 340 m/s in air). Even if there were air, the flash would be seen first and the sound would be heard later, not at the same time.

Answer
There should be no sound in space, and sound is never heard at the same time as the flash, because light travels much faster.
Q9A source produces a sound wave of wavelength 3.44 m. If the wave travels with a speed of 344 m s⁻¹ find its time period.▾

Given: wavelength λ = 3.44 m, speed v = 344 m/s

To find: time period T

In one time period, the wave travels one wavelength, so v = λ / T.

\[T = \dfrac{\lambda}{v} = \dfrac{3.44}{344} = 0.01\text{ s}\]
Answer
The time period is 0.01 s (frequency 100 Hz).
Q10A ship searching for a sunken ship sent a sonar signal and detected an echo after 5 s. If ultrasonic wave travels at 1525 m s⁻¹ in seawater, approximately how far down in the ocean is the wreckage of the sunken ship located?▾

Given: total time = 5 s, speed v = 1525 m/s

To find: depth of the wreck

The time to reach the wreck = 5/2 = 2.5 s.

\[d = v \times t = 1525 \times 2.5 = 3812.5\text{ m}\]
Answer
The wreckage is about 3812.5 m (nearly 3.8 km) below the surface.
Q11A vehicle is fitted with an ultrasonic distance sensor as part of parking assistance system which provides echolocation, while the driver is reversing the vehicle. It emits ultrasonic wave (about 40 kHz) which is reflected by the obstacle. When the warning beep starts sounding at a distance of 1.2 m from the obstacle, how much time is taken by ultrasonic wave to travel to the obstacle and come back? Assume the speed of ultrasonic wave in air to be 345 m s⁻¹.▾

Given: distance of obstacle = 1.2 m, speed v = 345 m/s

To find: time taken to go to the obstacle and come back

The wave travels to the obstacle and back, so the total distance = 2 × 1.2 = 2.4 m.

\[t = \dfrac{2.4}{345} = 0.00696\text{ s}\] \[\approx 7 \times 10^{-3}\text{ s}\]
Answer
The wave takes about 0.007 s (7 ms).
Q12The speed of sound in air is about 331 m s⁻¹ at 0 ºC and nearly 344 m s⁻¹ at 22 ºC. Roughly how much extra time will the sound of thunder take to travel a distance of 1720 m, if the air temperature changes from 22 ºC to 0 ºC? Assume that all other conditions remain unchanged.▾

Given: distance = 1720 m; speed at 22 °C = 344 m/s; speed at 0 °C = 331 m/s

To find: extra time taken at 0 °C

At 22 °C:

\[t_1 = \dfrac{1720}{344} = 5\text{ s}\]

At 0 °C:

\[t_2 = \dfrac{1720}{331} = 5.196\text{ s}\]

Extra time:

\[t_2 - t_1 = 5.196 - 5 = 0.196\text{ s}\]
Answer
The sound takes roughly 0.2 s longer at 0 °C.
Q13The variation of density of medium for a sound wave propagating with a speed of 340 m s⁻¹ is shown in Fig. 10.32. Calculate the wavelength and frequency of the sound wave.▾

Given: speed v = 340 m/s

In Fig. 10.32, the arrow of length 8 cm runs from the centre of the first compression to the centre of the third compression.

From one compression to the next is one wavelength, so 8 cm covers 2 wavelengths.

C C C R R R R 8 cm = 2λ www.boundlessmaths.com
Fig. 10.32 (redrawn): C = compression, R = rarefaction
\[2\lambda = 8\text{ cm}\] \[\lambda = 4\text{ cm} = 0.04\text{ m}\]

Using v = λ × ν

\[\nu = \dfrac{v}{\lambda} = \dfrac{340}{0.04} = 8500\text{ Hz}\]
Answer
Wavelength = 4 cm and frequency = 8500 Hz (8.5 kHz).
Q14The graphical representation of two sound waves A and B propagating at the same speed of 345 m s⁻¹ is shown in Fig. 10.33. What is the wavelength of each of them? Also, calculate their frequencies.▾

Given: speed of both waves v = 345 m/s

From the graph, wave A completes 3 full waves in 7.5 cm, and wave B completes 1.5 waves in 7.5 cm. So:

0 2.5 5.0 7.5 Distance (cm) Density A B www.boundlessmaths.com
Fig. 10.33 (redrawn): wave A completes 3 waves in 7.5 cm, wave B completes 1.5 waves
\[\lambda_A = \dfrac{7.5}{3} = 2.5\text{ cm} = 0.025\text{ m}\] \[\lambda_B = \dfrac{7.5}{1.5} = 5.0\text{ cm} = 0.05\text{ m}\]

Using ν = v / λ:

AWave A
\[\nu_A = \dfrac{345}{0.025} = 13800\text{ Hz}\]
Ans.λ = 2.5 cm, ν = 13800 Hz
BWave B
\[\nu_B = \dfrac{345}{0.05} = 6900\text{ Hz}\]
Ans.λ = 5.0 cm, ν = 6900 Hz
Q15Two identical sound sources are placed at A and B — one in air and one submerged in water (Fig. 10.34). Both produce sounds at the same time, which travel horizontally to the vertical side of the cliff and come back. If the time taken by the sound to return to A is 4.5 times than that of B, what is the ratio between the speeds of sound in air and water?▾

Let the distance from each source to the cliff be d. Each sound travels 2d (to the cliff and back).

Let v₁ = speed in air (source A) and v₂ = speed in water (source B).

A B air water same distance d cliff www.boundlessmaths.com
Both sounds travel the same distance d to the cliff and back (total 2d)
\[t_A = \dfrac{2d}{v_1}, \quad t_B = \dfrac{2d}{v_2}\]

Given: t_A = 4.5 × t_B

\[\dfrac{2d}{v_1} = 4.5 \times \dfrac{2d}{v_2}\]

Cancel 2d from both sides:

\[\dfrac{1}{v_1} = \dfrac{4.5}{v_2}\]

Rearranging:

\[\dfrac{v_1}{v_2} = \dfrac{1}{4.5} = \dfrac{2}{9}\]
Answer
The ratio of the speed of sound in air to that in water is 2 : 9 (that is, 1 : 4.5).
Section H

The Journey Beyond

5 Questions
JB1Many people use earphones extensively these days. Find out the research studies that might have been done to understand the impact of excessive use of earphones on hearing (if any). Also, find out how hearing is tested and what are the decibel ranges for defining mild, moderate and severe hearing loss. What are the government schemes for purchasing or fitting of aids or appliances and free cochlear implants? Write an article on your findings.▾

A sample article (points to include):

1. Effect of earphones: Studies by health bodies, such as the World Health Organization (WHO), report that listening to loud music for a long time through earphones can damage the ear and cause permanent hearing loss, especially in young people. Safe listening habits are to keep the volume below about 60 % of the maximum and to take breaks.

2. How hearing is tested: A hearing test called audiometry is done by an audiologist. The person listens to pure tones of different frequencies and loudness through headphones and signals when a tone is heard. The result is plotted as an audiogram.

3. Decibel ranges (hearing level, one commonly used scale):

Degree of hearing lossHearing level (dB)
Mild26 to 40
Moderate41 to 55
Moderately severe56 to 70
Severe71 to 90
Profoundabove 90

4. Government schemes: The scheme ADIP (Assistance to Disabled Persons for Purchase/Fitting of Aids and Appliances) of the Government of India supports hearing aids and other aids, and also covers cochlear implants for young children with severe hearing loss. The National Programme for Prevention and Control of Deafness (NPPCD) also works on screening and treatment. The eligibility rules change from time to time, so check the official websites before writing the final article.

Answer
The article should cover the effect of loud earphone use, hearing tests (audiometry), decibel ranges of hearing loss, and the government schemes. Use your own research and the latest official sources.
JB2Make a cone using a poster paper or cardboard and adhesive tape. Cover a mobile phone that is playing music with the cone. Compare the loudness of the sound with and without the cone. You can also use another mobile phone with an app to measure the characteristics of the sound in both cases. Try experimenting with different shapes and record your observations. (This activity is to be facilitated by the teacher.)▾

Procedure: Make a cone from poster paper, with a small opening at the narrow end. Place the phone playing music at the narrow end and listen from the wide end. Then listen without the cone from the same distance.

Expected observation: With the cone, the sound is louder in front of the wide opening than without the cone.

Reason: The walls of the cone reflect the sound waves again and again, and send them forward in one direction, instead of letting them spread out in all directions. This is the principle of a megaphone.

Different shapes: A cone with a wider mouth or a longer cone directs the sound better. A shape that does not guide the sound forward, such as a flat sheet, makes little difference.

Answer
The cone makes the sound louder in the forward direction, because it reflects the sound and directs it, so the sound does not spread out in all directions.
JB3How does the curved design of ceilings and walls behind the stage in concert and conference halls improve the quality of sound for the audience compared to flat surfaces? You may consult an architect or search it on the internet.▾

A curved surface behind the stage reflects the sound coming from the stage towards the audience.

A flat surface reflects sound in only one fixed direction, and the reflected sound may not reach all parts of the hall.

A curved ceiling and wall spread the reflected sound evenly over the whole audience, so even the people sitting at the back hear clearly.

The design also reduces unwanted echoes and reverberation, so the speech and music are clear.

Answer
Curved surfaces reflect and spread the sound evenly to the whole audience and reduce echoes. Flat surfaces do not do this well.
JB4Carry out a simple activity to measure the speed of sound, along with a friend in a large open ground of size 200 m or more. (This activity is to be facilitated by the teacher.)(i)Your friend stands at one end of the open ground with the balloons, while you stand at the other end with the stopwatch.(ii)Signal your friend to burst one balloon. When you see the balloon burst, start the stopwatch. As soon as you hear the ‘pop’ sound of the bursting balloon, stop the timer and note down the reading.(iii)Repeat this experiment multiple times and take the average value of the times noted.(iv)Note the approximate distance between you and your friend using a map application on a mobile phone.(v)Divide the distance measured with the average time to get the average speed of sound. What value of speed did you get from the experiment? Compare it with the speed of sound in air, which is typically about 346 m s⁻¹ at 25 °C.(vi)Why did you measure the time between ‘seeing’ and ‘hearing’ the balloon burst?▾

Sample readings: distance = 250 m. The times noted: 0.72 s, 0.74 s, 0.73 s, 0.73 s and 0.73 s.

Average time:

\[\dfrac{0.72+0.74+0.73+0.73+0.73}{5}\] \[= 0.73\text{ s}\]

(v) Speed of sound:

\[v = \dfrac{250}{0.73} = 342.5\text{ m/s}\]

This is close to the typical value of 346 m/s. A small difference arises from errors in the reaction time of starting and stopping the stopwatch and in measuring the distance.

(vi) Why measure the time between seeing and hearing: Light travels at 300000 km/s, so we see the burst almost at the same instant it happens. The time between seeing and hearing is the time taken by sound to travel the distance. If we started the stopwatch when the friend gave the signal, the time taken by the signal would be added and the result would be wrong.

Answer
Speed of sound = distance / average time (about 342 m/s in the sample readings). The time is measured between seeing and hearing because light reaches us almost instantly.
JB5Explore the internet resources to explore the effect of humidity and temperature on the speed of sound. Some such resources are:
(i) https://phet.colorado.edu/en/simulations/sound-waves/
(ii) https://musiclab.chromeexperiments.com/Experiments
(iii) https://phyphox.org/experiments
▾

Effect of temperature: The speed of sound in air increases when the temperature increases. For example, it is about 331 m/s at 0 °C and about 344 m/s at 22 °C.

Effect of humidity: The speed of sound in air increases when the humidity increases.

Reason: At a higher temperature, the particles of air move faster, so the disturbance is passed on from particle to particle more quickly.

Answer
The speed of sound in air increases with an increase in temperature and with an increase in humidity.
💡 Chapter 10's core idea, in one line

Sound is a vibration that becomes a travelling disturbance of compressions and rarefactions in a medium — carrying energy but not matter — and every property we can measure about it (wavelength, frequency, time period, amplitude, and speed, tied together by v = λν) explains what we hear as pitch and loudness, why sound reflects as echo or reverberation, and how frequencies beyond our own hearing, from a bat's ultrasonic call to a ship's SONAR ping, let us sense what our ears alone cannot.

Extra Practice

The Practice Continues

7 Questions

Seven extra questions in the style of the textbook's own activities and examples, for independent practice once you've gone through everything above. Attempt each one on paper first, then tap to check.

EP1A sound wave has a frequency of 250 Hz and travels through air at 340 m s⁻¹. Find its wavelength.▾

Given: ν = 250 Hz, v = 340 m/s

To find: wavelength λ

\[\lambda = \dfrac{v}{\nu} = \dfrac{340}{250} = 1.36\text{ m}\]
Answer
The wavelength is 1.36 m.
EP2A ship sends a SONAR signal that returns as an echo after 6 seconds. If the speed of sound in seawater is 1500 m s⁻¹, find the depth of the sea at that place.▾

Given: total time = 6 s, v = 1500 m/s

To find: depth of the sea

Time to reach the bottom = 6/2 = 3 s.

\[d = 1500 \times 3 = 4500\text{ m}\]
Answer
The depth of the sea is 4500 m (4.5 km).
EP3Two sounds have the same amplitude but different frequencies: one at 200 Hz and one at 2000 Hz. Will they sound equally loud? Will they sound the same? Explain.▾

Loudness depends mainly on the amplitude of the wave. Both waves have the same amplitude, so they carry about the same energy, and they will sound about equally loud.

Pitch depends on frequency. The 2000 Hz sound has a higher frequency, so it has a higher pitch (sounds shriller), and the 200 Hz sound has a lower pitch (sounds deeper).

Answer
They will be about equally loud, but they will not sound the same, because their pitch is different.
EP4A wave has a time period of 0.02 seconds. Find its frequency, and state whether this frequency is audible to humans.▾

Given: T = 0.02 s

To find: frequency, and whether it is audible

\[\nu = \dfrac{1}{T} = \dfrac{1}{0.02} = 50\text{ Hz}\]

The audible range is 20 Hz to 20000 Hz, and 50 Hz lies in this range.

Answer
The frequency is 50 Hz, which is audible to humans.
EP5A man standing between two parallel cliffs fires a gun. He is 340 m from the first cliff and 510 m from the second cliff. He hears two echoes. Find the time interval between the two echoes. (Speed of sound = 340 m s⁻¹)▾

Given: distances = 340 m and 510 m; v = 340 m/s

To find: time interval between the two echoes

Each sound goes to a cliff and back, so the total distance = 2d.

Echo from the first cliff:

\[t_1 = \dfrac{2 \times 340}{340} = 2\text{ s}\]

Echo from the second cliff:

\[t_2 = \dfrac{2 \times 510}{340} = 3\text{ s}\]

Time interval:

\[t_2 - t_1 = 3 - 2 = 1\text{ s}\]

1 s is more than 0.1 s, so the two echoes are heard separately.

Answer
The two echoes are heard 1 s apart (the first after 2 s and the second after 3 s).
EP6A tuning fork of frequency 512 Hz produces sound which travels from air into water. Find the wavelength of the sound in air and in water. What stays the same when the sound goes from air into water? (Speed of sound: air 340 m s⁻¹, water 1500 m s⁻¹)▾

Given: ν = 512 Hz; speed in air = 340 m/s; speed in water = 1500 m/s

Using λ = v / ν:

(i)Wavelength in air
\[\lambda_{air} = \dfrac{340}{512} = 0.664\text{ m}\]
Ans.0.664 m
(ii)Wavelength in water
\[\lambda_{water} = \dfrac{1500}{512} = 2.93\text{ m}\]
Ans.2.93 m

The frequency is decided by the source (the tuning fork), so it stays the same at 512 Hz. The speed changes with the medium, so the wavelength also changes.

Answer
Wavelength is 0.664 m in air and 2.93 m in water. The frequency (512 Hz) stays the same.
EP7A large empty hall sounds “echoey” with claps lingering after you clap, while a small room with curtains and carpets sounds “dead.” Explain this difference.▾

Large empty hall: It has hard, smooth walls, floor and ceiling that reflect sound well. Sound is reflected many times from these surfaces. Because the hall is large, the reflections reach us at slightly different times, so the sound persists after the clap stops (reverberation).

Small room with curtains and carpets: Soft, porous surfaces such as curtains and carpets absorb sound instead of reflecting it, so very little sound is reflected back. Also, in a small room the reflections come back so quickly that they cannot be separated from the original sound.

This is why concert halls use absorbing panels, curtains and upholstered chairs to control reverberation.

Answer
Hard surfaces in a large hall reflect sound many times, so it lingers. Soft surfaces in a small room absorb the sound, so it dies out quickly.
Common Questions

Frequently Asked Questions

Sound travels faster through air at higher temperatures because warmer air molecules move faster and collide with each other more frequently, transmitting the vibrations of a sound wave more quickly from particle to particle. This is why the speed of sound in air is often quoted at a specific temperature (around 343 m/s at 25°C), and changes noticeably as the temperature changes.
Sound is a mechanical wave, meaning it needs a material medium — solid, liquid, or gas — to travel. It moves by making particles of the medium vibrate and pass that vibration on to neighbouring particles. In a vacuum there are no particles at all, so there's nothing to vibrate and carry the sound wave forward, which is why space is completely silent despite what movies show.
Loudness depends on the amplitude of a sound wave — a larger amplitude means a louder sound, which is what changes when you turn up the volume. Pitch depends on frequency — a higher frequency means a higher-pitched sound, like a mosquito's whine, while a lower frequency means a deeper sound, like a truck's horn. These two properties are completely independent: a sound can be loud and low-pitched, quiet and high-pitched, or any combination of the two.
An echo is only heard if the reflecting surface is far enough away — at least about 17.2 m in air — for the reflected sound to arrive back at least 0.1 second after the original, which is the minimum gap our ears can distinguish as two separate sounds. Most rooms are smaller than this minimum distance, so the reflected sound arrives too quickly to be heard separately — it just blends with the original sound, making the room feel more "full" rather than producing a distinct echo.
The sound travels to the obstacle and back, so the total path is 2d = v × t and the distance is d = v × t ÷ 2. For the SONAR question, use the round-trip time and halve the distance. The ear can separate an echo only if it returns after a short delay; for the 0.2 s in P12 and a speed of about 340 m/s, the reflecting surface must be at least 34 m away.
Humans hear roughly 20 Hz to 20,000 Hz. Waves below 20 Hz are infrasonic (used by elephants and recorded from earthquakes), and waves above 20,000 Hz are ultrasonic. Ultrasound is used in SONAR, in bat echolocation and in medical ultrasound imaging, because high-frequency waves can be sent in narrow beams and reflect clearly.
Keep Going

Keep Exploring Class 9 Science

Browse the full list of Class 9 Science (Exploration) NCERT Solutions chapters, visit the Class 9 Science hub, or revise with the Class 9 Science Notes, or test yourself with the free Class 9 Science Sample Paper and Marking Scheme.

Expert CBSE Coaching · Class 9–12