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Class XI · Physics · Unit 10 · Interactive Lecture

Waves & Sound

The complete lecture — every wave comes alive in the live panel on the right as you read. Scroll down; the dark stage keeps pace: travelling waves, compressions, beats throbbing, strings standing still in loops, and a resonance tube finding the speed of sound.

A wave is a travelling disturbance that carries energy and momentum through a medium without any net transport of the medium. At Clifton beach the swell rolls in for kilometres, yet a floating bottle only bobs in place — the water stays, the energy arrives.

  • Mechanical waves — need a medium: water waves, sound, waves on a string.
  • Electromagnetic waves — need none: light and radio cross empty space at 3 × 10⁸ m/s.

Each particle of the medium does SHM about its own mean position; only the pattern moves on. In a transverse wave the particle motion is perpendicular to the wave's travel — crests and troughs, like a shaken rope or a sitar string.

Exam point: a cork on water ripples never travels with the wave — it oscillates about a fixed point.

In a longitudinal wave the particles oscillate parallel to the wave's direction, making travelling zones of compression (bunched) and rarefaction (spread out) — push-pull a Slinky along its length and watch the coil-bunches run.

TransverseLongitudinal
Particle motion⊥ to wave∥ to wave
Patterncrests & troughscompressions & rarefactions
Examplesstring, water surface, lightsound in air, Slinky push-pulse
Exam point: sound in air is always longitudinal — a gas has no sideways rigidity to carry a transverse wave.
  • Amplitude — maximum displacement from the mean position; energy ∝ A².
  • Wavelength λ — crest-to-crest distance, one full wave (m).
  • Period T & frequency f — time for one vibration; f = 1/T vibrations per second (Hz).
The wave equationin one period the wave advances one wavelength → v = λ/T
v = f λ — true for water, sound and light alike
worked — tabla note
f = 250 Hz, v = 340 m/s. λ?
λ = v/f = 340/250 = 1.36 m · T = 1/f = 4 ms

A vibrating tabla skin pushes air into a compression, then leaves a rarefaction as it swings back. These pressure pulses travel out as a longitudinal wave; the air itself only shivers in place.

  • Sound needs a medium — bell-jar experiment: pump the air out and the ringing bell falls silent though the hammer still strikes.
  • Audible range — 20 Hz to 20 000 Hz; above is ultrasonic (bats, ultrasound scans).
Speed of soundat 0 °C ≈ 331 m/s · at 20 °C ≈ 343 m/s
v ≈ 331 + 0.61 T (T in °C) — hotter air → faster sound
solids > liquids > gases: steel ≈ 5000, water ≈ 1480, air ≈ 343 m/s
worked — hot Karachi afternoon
v at 35 °C?
v = 331 + 0.61 × 35 ≈ 352 m/s
CharacteristicDepends onEveryday meaning
Loudnessamplitude (I ∝ A²)whisper vs shout
Pitchfrequencychild's voice high, man's voice low; thin sitar string vs thick
Qualitywaveform (mix of overtones)flute vs sitar on the same note still sound different

Loudness is compared on the decibel scale: 0 dB threshold of hearing, ~60 dB conversation, ~120 dB pain — a rickshaw horn at your ear.

Exam trap: pitch ↔ frequency, loudness ↔ amplitude. Never swap them.

Principle of superposition: where waves overlap, the resultant displacement is the sum of the individual displacements — then the waves pass on unchanged.

  • Constructive — crest on crest (in phase): A = A₁ + A₂. Path difference = .
  • Destructive — crest on trough (out of phase): A = |A₁ − A₂| → silence if equal. Path difference = (n + ½)λ.

Two loudspeakers on one signal make loud-and-quiet bands across a room; two ripple-tank dippers draw the same pattern in water. Noise-cancelling headphones are deliberate destructive interference.

Two notes of slightly different frequencies slide in and out of phase: in phase → loud, out of phase → quiet. The periodic throb of loudness is a beat.

Beat frequencyf_beat = |f₁ − f₂| throbs per second (distinct only below ~10 Hz)

Tuning by beats: the sitar or tabla player sounds the instrument against a harmonium note or tuning fork. Beats heard → out of tune; the player tightens the string or taps the gajra until the beats slow and vanish — zero beats means perfectly tuned.

worked — tuning a sitar string
440 Hz fork + string → 4 beats/s; tightening slows the beats. Original f?
f = 440 ± 4; tightening raised f and beats fell → f was below → 436 Hz

Two identical waves travelling in opposite directions (a wave and its reflection) superpose into a stationary wave: the pattern stops travelling and the string vibrates in fixed loops.

  • Node (N) — permanently still point; adjacent nodes are λ/2 apart.
  • Antinode (A) — maximum swing, midway between nodes; N→A = λ/4.
  • No net energy transfer — energy stays trapped, sloshing inside each loop.
String fixed at both ends (length L)L = n(λ/2) → fₙ = n v / 2L = n f₁, n = 1, 2, 3 …
v = √(F/m): tighter string → higher pitch (how a sitar is tuned)
worked — sitar string
L = 0.60 m, m = 1.0 × 10⁻³ kg/m, F = 90 N. f₁?
v = √(90/10⁻³) = 300 m/s → f₁ = v/2L = 300/1.2 = 250 Hz

Resonance: drive a body at its natural frequency and it responds with a large amplitude — a swing pushed in time, a glass shattered by a held note.

Board practical: a tuning fork of known f hums over a vertical tube while the water level is lowered. The trapped air column (closed at the water, open at the top) booms loudly when its length fits the wave:

Resonance tube (closed pipe)first boom: L₁ ≈ λ/4 · second boom: L₂ ≈ 3λ/4
λ = 2(L₂ − L₁) → v = f λ = 2 f (L₂ − L₁) — end-correction cancels
worked — speed of sound
f = 512 Hz, L₁ = 16.0 cm, L₂ = 49.5 cm. v?
λ = 2(0.495 − 0.160) = 0.670 m → v = 512 × 0.670 ≈ 343 m/s

Doppler effect: relative motion between source and observer changes the apparent frequency. Approaching → wavefronts bunch → higher pitch; receding → stretched → lower pitch. The ambulance on Sharea Faisal screams shriller coming towards you and drops to a deeper note the instant it passes — the siren itself never changed.

  • Radar speed guns and medical Doppler ultrasound use the same shift; galaxy red-shift is its light version.
  • Wave = energy transfer, no matter transfer; transverse ⊥, longitudinal ∥ (sound).
  • v = fλ; v_string = √(F/m); v_sound ≈ 331 + 0.61T m/s.
  • Loudness↔amplitude, pitch↔frequency, quality↔waveform.
  • Constructive nλ, destructive (n+½)λ; beats f_b = |f₁−f₂| → tuning.
  • Stationary: nodes λ/2 apart, fₙ = nf₁; resonance tube v = 2f(L₂−L₁).
🌊 Live panelWaves & Sound
Scroll the lecture — this panel animates each wave as you reach it.