Properties of Sound

Foundation

Sound is a longitudinal wave carried by the compressions and rarefactions of a medium — no sound in vacuum, about 340 m s⁻¹ in air. Loudness depends on amplitude, pitch on frequency and quality on waveform; echo ranging and ultrasonic sonar turn the wave equation into a way of measuring distances.

For:Secondary 5 Physics · Unit:Wave Motion · Lesson 5 of 6 in the learning path

After this lesson, you can:
  • Sound is a longitudinal wave of compressions and rarefactions; it needs a medium — a vacuum carries no sound
  • The speed of sound is about 340 m s⁻¹ in air; fastest in solids and slowest in gases, rising slightly with temperature
  • Loudness — amplitude; pitch — frequency; quality — waveform; the audible range is about 20 Hz to 20 kHz
文體:科學知識說明文有聲朗讀

文體小知識:科學知識說明文——以縱波的角度重新認識聲音:傳播需要介質、空氣聲速約每秒 340 米,響度、音調與音色對應振幅、頻率與波形,並介紹回聲測距、超聲波與噪音分貝。

物理Physics
Before this lesson you should know: Reflection and Refraction of Light

§Text Passage

1Strike a tuning fork and its prongs vibrate back and forth, pushing and pulling the nearby air: squeezed regions become compressions and stretched regions rarefactions, and this alternating pattern travels outward as a wave, entering the ear and vibrating the eardrum. Sound is a longitudinal wave — the vibration is parallel to the direction of travel. Propagation needs a medium: put a ringing alarm clock inside a glass jar and pump out the air, and the ringing fades away — vacuum carries no sound.

2The speed of sound depends on the medium: fastest in solids, where particles are tightly bound; slower in liquids; slowest in gases. In air it is about 340 m per second, in water about 1500 m per second and in steel over 5000 m per second. Higher temperature speeds the air particles up and slightly raises the speed. For example, thunder follows lightning: if the gap is three seconds, the strike is about 340 × 3 = 1020 m away — the classic way to estimate a storm's distance.

3The audible frequency range runs from about 20 Hz to 20 kHz, and the upper limit falls with age. Sound above 20 kHz is ultrasound, below 20 Hz infrasound — both inaudible. The three subjective features of a note each map onto a physical quantity: loudness is set by amplitude, pitch by frequency, and quality (timbre) by waveform, which is why we can tell a piano from a guitar playing the same note.

4Sound reflects off obstacles, and the reflected sound is an echo. In echo ranging, distance equals speed of sound times time, divided by two, because the sound travels there and back. Ultrasound extends the idea: a ship's sonar pulses ultrasound at the seabed and times the echo to chart the depth; hospital B-scans send ultrasound through the body, and the reflections from different tissues build an image of a fetus. Ultrasound's high frequency and short wavelength give it directionality and precision.

5Noise is sound that annoys or harms, and its strength is measured in decibels: 0 dB is about the threshold of hearing, a conversation about 60 dB, and prolonged exposure above 80 dB damages hearing; concerts and pile-driving can exceed 110 dB. Ear plugs, volume limits and noise barriers all protect hearing, and decibels measure loudness level, never pitch — a favourite exam distinction.

1Summary 重點摘要

Sound is a longitudinal wave carried by the compressions and rarefactions of a medium — no sound in vacuum, about 340 m s⁻¹ in air. Loudness depends on amplitude, pitch on frequency and quality on waveform; echo ranging and ultrasonic sonar turn the wave equation into a way of measuring distances.

2Vocabulary cards Vocabulary

m
medium介質

The substance sound travels through, such as air, water or steel; a vacuum carries no sound.

s
speed of sound聲速

The speed at which sound travels; about 340 m s⁻¹ in air, rising slightly with temperature.

e
echo回聲

Sound reflected back from an obstacle; useful for measuring distances.

a
audible frequency range可聞頻率範圍

The range of frequencies the human ear can hear, about 20 Hz to 20 kHz.

u
ultrasound超聲波

Sound with frequency above 20 kHz, inaudible to humans; used in sonar and B-scans.

l
loudness響度

How strong a sound is, set by amplitude — larger amplitude, louder sound.

p
pitch音調

How high a note is, set by frequency — higher frequency, higher pitch.

q
quality (timbre)音色

The character of a sound, set by its waveform, letting us tell instruments apart.

d
decibel分貝

The unit of sound intensity level; 0 dB is about the threshold of hearing, and prolonged exposure above 80 dB harms hearing.

s
sonar聲吶

A system that sends ultrasound pulses and times the echoes to locate objects underwater.

3Step by step Steps

  1. Step 1: How sound is made and travelsEvery sound starts with a vibration: a tuning fork, vocal folds or a guitar string pushes and pulls the surrounding air, forming alternating compressions and rarefactions — a longitudinal wave that spreads outward. Sound needs a medium: vacuum carries none. For example, put a ringing electric bell inside a glass jar and pump the air out: the ringing fades to almost nothing while the hammer is still striking — proof that sound needs air to reach our ears, while light is unaffected and we can still see the bell moving.
  2. Step 2: Speed of sound, medium and temperatureThe speed of sound depends on the medium: particles bound most tightly in solids pass the vibration on fastest, and gases are slowest. Typical values: about 340 m s⁻¹ in air, about 1500 m s⁻¹ in water, and over 5000 m s⁻¹ in steel. Raising the temperature makes air particles move faster and slightly increases the speed. For example, put your ear to a rail and you hear an approaching train earlier than through the air, because steel carries sound more than ten times faster; soldiers of old slept with quivers on the ground to hear riders coming through the earth.
  3. Step 3: Audible range and ultrasoundThe human ear hears roughly 20 Hz to 20 kHz; the upper limit is higher in children and falls with age, so many elders cannot hear the high-pitched beeps of electronics. Above 20 kHz is ultrasound; below 20 Hz is infrasound — both inaudible. Bats and dolphins use ultrasound to navigate and communicate; earthquakes and storms produce infrasound. For example, anti-mosquito devices emit tones near 20 kHz that most adults cannot hear while some teenagers can — a neat demonstration that the audible range differs from person to person.
  4. Step 4: Loudness, pitch and qualityThree features of a note map onto three physical quantities: loudness to amplitude, pitch to frequency, quality (timbre) to waveform. Pluck a string harder and the amplitude grows — the note is louder; shorten or tighten the string and the frequency rises — the pitch is higher; the same note on a piano and a trumpet has different waveforms, hence different timbres. For example, a piano tuner tells instruments apart by timbre, and a doctor distinguishes heartbeats from murmurs the same way; turning up a radio raises the amplitude and loudness only — it never turns a man's voice into a woman's, because frequency and waveform are unchanged.
  5. Step 5: Echo ranging — remember to halveSound reflected from an obstacle is an echo. In echo ranging, distance = (speed of sound × time) ÷ 2, because the sound goes there and back. For example, shout at a cliff and hear the echo 1.5 s later: the one-way time is 0.75 s, so the cliff stands 340 × 1.5 ÷ 2 = 255 m away. The ear can only separate an echo from the original if the gap exceeds about 0.1 s, meaning the obstacle is at least some 17 m off; in an ordinary classroom the walls are too near, the echo blends into reverberation, and no distinct echo is heard.
  6. Step 6: Applications of ultrasoundUltrasound has high frequency and short wavelength, so it forms narrow, directional beams — ideal for precise probing. Ship sonar pulses ultrasound at the seabed and times the echo to chart depth; fishing boats find shoals the same way; hospital B-scans image fetuses and organs with no radiation; industry tests metal castings for hidden cracks. For example, if sonar receives the seabed echo 2 s after the pulse, the water depth is 1500 × 2 ÷ 2 = 1500 m; substituting 340 m s⁻¹ from air would be badly wrong, because the speed of sound in water is entirely different.
  7. Step 7: Noise, decibels and ear protectionNoise is unwanted or harmful sound, and its strength is given in decibels: 0 dB is roughly the threshold of hearing, 30 dB a whisper, 60 dB conversation; prolonged exposure above 80 dB damages hearing, and above 120 dB can injure immediately. Decibels measure loudness level, not frequency — a favourite exam distinction. For example, ear plugs cut the sound reaching your ears by 20–30 dB and should be worn by construction workers, musicians and frequent flyers; playing earphones at maximum volume likewise causes permanent hearing loss over time.

4Diagrams Diagrams

♪喇叭傳播方向密 compression疏 rarefaction聲 = 縱波,需要介質空氣中約 340 m s⁻¹(15°C)真空不能傳聲響度=振幅 音調=頻率回聲測距:距離 = 340 × t ÷ 2超聲波:聲吶、B 超、潔牙頻率範圍約 20 Hz–20 kHz(人耳可聽);超過 20 kHz 為超聲波。
Fig. 1: Sound as a longitudinal wave

5Worked example Example

Example: while camping, a camper shouts towards a cliff and hears a clear echo 1.5 s later. The speed of sound is 340 m s⁻¹. (a) Find the distance to the cliff. (b) A fishing boat's sonar sends an ultrasound pulse to the seabed and receives the echo 0.8 s later; taking the speed of sound in sea water as 1500 m s⁻¹, find the sea depth.

  1. (a) The sound makes a round trip in 1.5 s; one-way time = 1.5 ÷ 2 = 0.75 s
  2. (a) Distance = speed × one-way time = 340 × 0.75
  3. (a) Distance = 255 m
  4. (b) One-way time in sea water = 0.8 ÷ 2 = 0.4 s
  5. (b) Depth = 1500 × 0.4 = 600 m
  6. Answer: (a) Distance = 340 × 1.5 ÷ 2 = 255 m. (b) Depth = 1500 × 0.8 ÷ 2 = 600 m. In both parts the key is halving the round-trip time; the other point is that part (b) must use 1500 m s⁻¹ for sea water — change the medium and the speed changes, the classic trap in echo-ranging problems.

6Common mistakes Mistakes

✗ Believing sound can travel through a vacuum.
✓ Sound is the vibration of a medium's particles; a vacuum has none to vibrate, which is why the ringing fades in the evacuated jar.
✗ Forgetting to halve the time in echo ranging.
✓ The measured time is there and back: distance = speed × time ÷ 2; without halving, distances come out doubled.
✗ Thinking a louder sound has a higher frequency.
✓ Loudness is set by amplitude and pitch by frequency; turning up the volume does not change the frequency.
✗ Reading ultrasound as an especially loud sound.
✓ Ultrasound means frequency above 20 kHz — a matter of frequency, not loudness, and inaudible to humans.
✗ Taking the decibel as a unit of frequency.
✓ The decibel measures sound intensity (loudness) level; the unit of frequency is the hertz — unrelated quantities.

7Quick check Quick check

Q1Why can a vacuum transmit no sound?

Q2An echo returns 2 s after a shout; the speed of sound is 340 m s⁻¹. How far is the cliff?

Q3What determines loudness, pitch and quality?

Q4What is ultrasound? Give two applications.

Q5With sound at 1500 m s⁻¹ in water, a sonar echo returns 1 s after the pulse. How deep is the sea?

8Recap Recap

  • Sound is a longitudinal wave of compressions and rarefactions; it needs a medium — a vacuum carries no sound
  • The speed of sound is about 340 m s⁻¹ in air; fastest in solids and slowest in gases, rising slightly with temperature
  • Loudness — amplitude; pitch — frequency; quality — waveform; the audible range is about 20 Hz to 20 kHz
  • Echo ranging: distance = speed × time ÷ 2; the speed changes with the medium
  • Ultrasound (above 20 kHz) powers sonar and B-scans; noise is measured in decibels, and exposure above 80 dB harms hearing

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