Waves explains how energy and momentum travel through a medium without the medium itself moving along, covering transverse and longitudinal waves, the master relation v = f times lambda, and the speed of waves on strings and of sound in gases. It then builds to superposition, standing waves with nodes and antinodes, harmonics in strings and air columns, beats, and the Doppler effect. For NEET it is a steady-scoring chapter where standing waves, organ pipes, beats, and Doppler regularly appear, so getting the formulas and sign conventions right is what separates a clean answer from a careless slip.
Table of Contents
- Key Concepts - wave types, progressive waves, wave speed, sound, superposition, standing waves, beats, Doppler
- Weightage in Board & Entrance Exams
- Important Definitions
- Solved Examples
- Important Questions for Board Exams
- Quick Revision Points
Key Concepts
1. What is a Wave?
A wave is a disturbance that travels through a medium, transporting energy and momentum from one point to another without any net transport of the medium itself. Drop a stone in a pond - the ripple spreads outward, but a floating leaf only bobs up and down; it does not move with the ripple.
Mechanical waves (water waves, sound, waves on a string) need a material medium to travel. Electromagnetic waves (light, radio) need no medium. This chapter deals mainly with mechanical waves.
2. Transverse and Longitudinal Waves
Waves are classified by the direction in which the particles of the medium vibrate relative to the direction the wave travels.
| Transverse Wave | Longitudinal Wave |
|---|---|
| Particles vibrate perpendicular to the direction of wave propagation | Particles vibrate parallel to the direction of wave propagation |
| Made of crests and troughs | Made of compressions and rarefactions |
| Example: wave on a string, ripples on water, light | Example: sound waves in air, waves in a spring (pushed lengthwise) |
| Can travel only in solids and on liquid surfaces | Can travel in solids, liquids and gases |
[DIAGRAM: A horizontal string showing crests and troughs (transverse) above a slinky showing alternating compressions and rarefactions (longitudinal), both with the wave-travel direction marked by an arrow.]
Key idea: Sound in air is always longitudinal because gases cannot sustain the shearing stress needed for a transverse wave.
3. Terms Used to Describe a Wave
- Amplitude (A): maximum displacement of a particle from its mean position.
- Wavelength (λ): distance between two consecutive points in the same phase (crest to crest, or compression to compression). SI unit: metre.
- Time period (T): time taken for one complete oscillation. Frequency f = 1/T, SI unit hertz (Hz).
- Angular frequency: ω = 2πf = 2π/T. Wave number: k = 2π/λ.
- Wave velocity (v): the speed at which the disturbance travels: v = fλ = ω/k.
4. Displacement Relation for a Progressive Wave
A progressive (travelling) wave moves continuously in one direction, carrying energy with it. For a sinusoidal wave travelling along the positive x-direction, the displacement y of a particle at position x and time t is:
y(x, t) = A sin(kx − ωt + φ)
- A = amplitude, k = 2π/λ = angular wave number, ω = 2πf = angular frequency, φ = initial phase (phase constant).
- For a wave travelling in the negative x-direction: y(x, t) = A sin(kx + ωt + φ).
- The term (kx − ωt) is the phase of the wave.
Phase difference and path difference: a path difference of one wavelength λ corresponds to a phase difference of 2π. So phase difference Δφ = (2π/λ) × path difference.
5. Speed of a Travelling Wave
The speed of a wave is fixed by the properties of the medium, not by how the wave was produced. The general result is v = fλ.
Speed of a Transverse Wave on a String
For a stretched string, the wave speed depends on the tension and how heavy the string is:
v = √(T/μ)
where T is the tension in the string and μ is the linear mass density (mass per unit length, kg/m). A tighter, lighter string carries waves faster - that is how a guitar is tuned.
Speed of a Longitudinal Wave
For a longitudinal wave in a medium of bulk modulus B and density ρ: v = √(B/ρ). In a solid rod (Young’s modulus Y): v = √(Y/ρ).
6. Speed of Sound - Newton’s Formula and Laplace’s Correction
Sound is a longitudinal wave, so its speed in a gas is v = √(B/ρ). The question is which bulk modulus B to use.
Newton’s Formula
Newton assumed that sound travels through air under isothermal conditions (constant temperature). Then B equals the pressure P, giving:
v = √(P/ρ)
For air at STP this gives about 280 m/s - but the measured value is about 332 m/s. Newton’s formula is roughly 15% too low.
Laplace’s Correction
Laplace pointed out that compressions and rarefactions happen so fast that there is no time for heat to flow - the process is adiabatic, not isothermal. The relevant bulk modulus is then γP, where γ = C_p/C_v is the ratio of specific heats (γ = 1.4 for air).
v = √(γP/ρ)
This gives about 332 m/s, matching experiment. Factors affecting speed of sound: it increases with temperature (v ∝ √T in kelvin), increases with humidity, but is independent of pressure (at constant temperature) and of frequency.
7. Principle of Superposition of Waves
When two or more waves travel through the same medium at the same time, the resultant displacement at any point is the vector sum of the displacements due to each individual wave.
y = y₁ + y₂ + y₃ + …
This single principle explains interference, standing waves, and beats. After they cross, each wave continues as if the other was never there.
8. Reflection of Waves
When a wave hits a boundary, part of it is reflected. What happens to the phase depends on the boundary.
- Reflection from a rigid (fixed) boundary: the wave is reflected with a phase change of π (180°). A crest returns as a trough. (Example: string fixed to a wall.)
- Reflection from a free (open) boundary: the wave is reflected with no phase change. A crest returns as a crest. (Example: open end of an organ pipe.)
9. Standing (Stationary) Waves
When two identical waves of the same frequency and amplitude travel in opposite directions and superpose, they form a standing wave - a pattern that appears to stand still instead of travelling.
The resultant of y₁ = A sin(kx − ωt) and y₂ = A sin(kx + ωt) is:
y = 2A sin(kx) cos(ωt)
- Nodes: points of permanently zero displacement, where 2A sin(kx) = 0. They occur at x = 0, λ/2, λ, … (spacing λ/2).
- Antinodes: points of maximum displacement (amplitude 2A). They occur halfway between nodes (spacing λ/2).
- Distance between a node and the nearest antinode is λ/4.
- A standing wave does not transport energy along the medium - energy stays trapped between the boundaries.
[DIAGRAM: A standing wave on a string showing fixed nodes (N) at the ends and along the string, with antinodes (A) bulging between them; node-to-node spacing labelled λ/2.]
10. Normal Modes of a Stretched String
A string fixed at both ends can vibrate only at certain frequencies, called its normal modes or harmonics, because both ends must be nodes.
For a string of length L, the allowed wavelengths are λ = 2L/n (n = 1, 2, 3…), so the frequencies are:
fₙ = n·v/2L = (n/2L)√(T/μ), where n = 1, 2, 3, …
- n = 1: fundamental frequency (first harmonic), f₁ = v/2L.
- n = 2: second harmonic (first overtone), f₂ = 2f₁.
- A string produces all harmonics - both even and odd - so its overtones are 2f₁, 3f₁, 4f₁, …
11. Normal Modes in Air Columns (Organ Pipes)
Sound waves form standing waves inside pipes. An open end is an antinode (free to vibrate) and a closed end is a node (cannot vibrate).
Open Pipe (open at both ends)
Both ends are antinodes. The allowed frequencies are:
fₙ = n·v/2L (n = 1, 2, 3, …)
An open pipe gives all harmonics (1f, 2f, 3f, …), which is why it sounds richer.
Closed Pipe (closed at one end)
The closed end is a node and the open end an antinode. The allowed frequencies are:
fₙ = n·v/4L (n = 1, 3, 5, … only odd)
A closed pipe gives only odd harmonics (1f, 3f, 5f, …). Its fundamental v/4L is half that of an open pipe of the same length.
| Pipe | Fundamental | Harmonics present |
|---|---|---|
| Open pipe | v/2L | All (1, 2, 3, 4…) |
| Closed pipe | v/4L | Only odd (1, 3, 5…) |
12. Beats
When two sound waves of slightly different frequencies superpose, the loudness rises and falls periodically. These periodic variations in intensity are called beats.
The number of beats heard per second equals the difference of the two frequencies:
Beat frequency = |f₁ − f₂|
- Beats are audible only if |f₁ − f₂| is less than about 10 Hz (the ear cannot resolve faster fluctuations).
- Used to tune musical instruments - when the beats vanish, the two notes are identical.
13. The Doppler Effect
The Doppler effect is the apparent change in the frequency (pitch) of a sound when the source, the observer, or both are moving relative to each other. An approaching ambulance sounds higher-pitched; as it moves away the pitch drops.
The general formula for the observed frequency f′ is:
f′ = f · (v ± v₀)/(v ∓ v_s)
where v is the speed of sound, v₀ the observer’s speed and v_s the source’s speed.
Sign Convention
- Take all velocities positive along the direction from source to observer.
- Use the top sign when source and observer move towards each other (frequency increases).
- Use the bottom sign when they move away from each other (frequency decreases).
Note: for light the Doppler shift gives the “red shift” of receding stars, but the sound formula above is not symmetric in v₀ and v_s - moving the source is not the same as moving the observer.
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Weightage in Board & Entrance Exams
| Exam | Typical Weightage | Most-Tested Areas |
|---|---|---|
| CBSE Board (Class 11) | 6–8 marks | Progressive wave equation, organ pipes, beats, Doppler effect |
| JEE Main / Advanced | 1–2 questions | Standing waves, string & pipe harmonics, Doppler numericals |
| NEET | 1–2 questions | Speed of sound, beats, Doppler effect, wave equation |
[TABLE: Question-type split - VSA (1 mark): wave types, definitions, beat frequency; SA (2–3 marks): wave equation, Newton-Laplace, pipe harmonics; LA (5 marks): standing-wave derivation, Doppler-effect derivation.]
Important Definitions
| Term | Definition |
|---|---|
| Wave | A disturbance that transfers energy through a medium without net transfer of matter |
| Transverse wave | Particles vibrate perpendicular to the direction of propagation (crests and troughs) |
| Longitudinal wave | Particles vibrate parallel to propagation (compressions and rarefactions) |
| Wavelength (λ) | Distance between two consecutive points in the same phase |
| Wave velocity | Speed at which the disturbance travels: v = fλ |
| Progressive wave | A wave that travels continuously transporting energy: y = A sin(kx − ωt) |
| Laplace’s correction | Sound propagates adiabatically, so v = √(γP/ρ) |
| Standing wave | Pattern formed by two opposite waves: y = 2A sin(kx) cos(ωt); no energy transport |
| Node / Antinode | Point of zero displacement / maximum displacement in a standing wave |
| Beats | Periodic rise and fall of loudness when two close frequencies superpose; rate = |f₁ − f₂| |
| Doppler effect | Apparent change in frequency due to relative motion of source and observer |
Solved Examples
Example 1
A wave has frequency 500 Hz and wavelength 0.66 m. Find its speed.
Answer: v = fλ = 500 × 0.66 = 330 m/s.
Example 2
A string of linear mass density 2 g/m is stretched with a tension of 80 N. Find the speed of a transverse wave on it.
Answer: μ = 2 g/m = 0.002 kg/m. v = √(T/μ) = √(80/0.002) = √40000 = 200 m/s.
Example 3
For a progressive wave y = 0.05 sin(20x − 600t) (SI units), find the amplitude, wave number, angular frequency, wavelength and speed.
Answer: A = 0.05 m; k = 20 rad/m; ω = 600 rad/s. λ = 2π/k = 2π/20 = 0.314 m. v = ω/k = 600/20 = 30 m/s.
Example 4
A pipe closed at one end has length 0.5 m. Taking the speed of sound as 340 m/s, find its fundamental frequency.
Answer: Closed pipe fundamental f = v/4L = 340/(4 × 0.5) = 340/2 = 170 Hz.
Example 5
Two tuning forks of frequencies 256 Hz and 260 Hz are sounded together. Find the beat frequency.
Answer: Beat frequency = |f₁ − f₂| = |256 − 260| = 4 Hz (4 beats per second).
Example 6
A source emitting sound of frequency 500 Hz moves towards a stationary observer at 30 m/s. Taking v = 330 m/s, find the apparent frequency.
Answer: Source approaching: f′ = f·v/(v − v_s) = 500 × 330/(330 − 30) = 500 × 330/300 = 550 Hz.
Important Questions for Board Exams
1-Mark Questions (VSA)
- Why can transverse waves not travel through gases?
- What is the phase difference corresponding to a path difference of one wavelength?
- State the relation between wave velocity, frequency and wavelength.
- Why does a closed organ pipe produce only odd harmonics?
- Two sound waves of frequencies 400 Hz and 404 Hz are sounded together. How many beats are heard per second?
2–3-Mark Questions (SA)
- State Newton’s formula for the speed of sound in air and explain Laplace’s correction.
- Distinguish between transverse and longitudinal waves with one example each.
- Derive the expression for the frequency of the nth harmonic of a string fixed at both ends.
- What are beats? Write the expression for beat frequency and state one use of beats.
5-Mark Questions (LA)
- Using the principle of superposition, derive the equation of a standing wave and obtain the positions of nodes and antinodes.
- Derive an expression for the apparent frequency heard by a stationary observer when the source of sound moves towards and then away from the observer (Doppler effect).
- Compare the modes of vibration of an open organ pipe and a closed organ pipe, deriving the frequencies of their harmonics.
Quick Revision Points
- Wave transfers energy, not matter; v = fλ = ω/k
- Transverse: ⟂ vibration, crests/troughs; Longitudinal: ∥ vibration, compressions/rarefactions
- Progressive wave: y = A sin(kx − ωt); k = 2π/λ, ω = 2πf
- Phase difference Δφ = (2π/λ) × path difference
- Wave on string: v = √(T/μ); longitudinal: v = √(B/ρ)
- Speed of sound - Newton: v = √(P/ρ); Laplace (adiabatic): v = √(γP/ρ); v ∝ √T
- Superposition: resultant displacement = sum of individual displacements
- Rigid boundary → phase change π; free boundary → no phase change
- Standing wave: y = 2A sin(kx) cos(ωt); node–node = λ/2, node–antinode = λ/4; no energy transport
- String (both ends fixed): fₙ = (n/2L)√(T/μ), all harmonics
- Open pipe: fₙ = nv/2L (all harmonics); Closed pipe: fₙ = nv/4L (odd harmonics only)
- Beats: beat frequency = |f₁ − f₂|, audible if < ~10 Hz
- Doppler: f′ = f(v ± v₀)/(v ∓ v_s); towards → higher pitch
Next Chapter: Class 12 Physics - Electric Charges and Fields
Class 11 Physics · Chapter 15 – swipe through all 9 cards to understand the whole chapter.
What a Wave Is
A wave carries energy and momentum through a medium without carrying matter.
Light is transverse; sound is longitudinal — never swap them.
- Transverse: particles vibrate perpendicular → crests & troughs
- Longitudinal: particles vibrate parallel → compressions & rarefactions
- The disturbance moves; the medium just wobbles in place
Wave Equation & v = fλ
One relation links speed, frequency and wavelength for every wave.
ω = 2πf, k = 2π/λ; minus sign → wave travels in +x.
- Read ω off the t-term, k off the x-term, then v = ω/k
- T = 1/f is the time period; A is the amplitude
- Across a new medium frequency stays fixed; v and λ change together
Speed of Mechanical Waves
Wave speed is set by the medium, not by frequency or amplitude.
μ in kg m⁻1 — convert g/cm → kg/m (the #1 silent error).
- String: more tension → faster; heavier string → slower
- Sound in gas (Laplace, adiabatic): v ∝ √T, v ∝ 1/√M
- Independent of pressure at fixed T; ≈ 332 m s⁻1 in air at 0°C
Superposition & Interference
When waves overlap, displacements add algebraically at every point.
Phase π ↔ path difference λ/2 → perfect cancellation.
- Constructive: path difference Δx = nλ (in phase, loud)
- Destructive: Δx = (n + ½)λ (out of phase, silent)
- After crossing, both waves carry on unchanged
Nodes & Antinodes
Two identical waves in opposite directions make a wave that stands still.
Adjacent nodes are λ/2 apart; node to nearest antinode is λ/4.
- Nodes: zero amplitude, permanently at rest
- Antinodes: maximum amplitude 2A
- No net energy crosses a node — it only sloshes within each loop
Strings & Open Pipes
A string fixed at both ends and an open pipe sustain all integer harmonics.
Fixed/closed end = node; free/open end = antinode.
- Fundamental f1 = v/2L; all harmonics 1f, 2f, 3f… present
- Rich tone (flute, guitar) from the full harmonic series
- For a string f ∝ √T — quadruple tension, frequency only doubles
Closed-Pipe Harmonics
A pipe closed at one end keeps only the odd harmonics.
Closed-pipe denominator is 4L, not 2L.
- Only odd harmonics 1f, 3f, 5f… → hollow, pure tone
- Open pipe’s fundamental is twice a closed pipe’s of equal length
- End correction ≈ 0.6r per open end raises effective length
Beats
Two nearly-equal frequencies make loudness swell and fade periodically.
Audible only if the gap ≤ ~10 Hz; same-direction waves.
- Unknown fork = f ± n — always two candidates
- Filing raises frequency; loading (wax) lowers it
- Fix the sign by whether beats grow or shrink after the change
Doppler Effect
Relative motion of source and observer shifts the perceived frequency.
Source speed always in the denominator; sanity-check approach → f’ > f.
- Approach raises pitch; recession lowers it
- v0: + toward source, − away · vₛ: − toward observer, + away
- Not symmetric for sound (medium fixes a frame); add wind w to v
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Frequently Asked Questions
In a transverse wave the particles of the medium vibrate perpendicular to the direction the wave travels, forming crests and troughs, as in waves on a string or light. In a longitudinal wave the particles vibrate parallel to the direction of travel, forming compressions and rarefactions, as in sound waves in air.
For any wave the speed equals frequency times wavelength, v = f times lambda, which can also be written v = omega divided by k. When a wave passes from one medium into another its frequency stays fixed, while its speed and wavelength change together.
Using Laplace’s adiabatic correction, the speed of sound in a gas is v = square root of (gamma times P divided by rho), and it is proportional to the square root of absolute temperature. It is independent of pressure at a fixed temperature, and in air at 0 degrees Celsius it is about 332 metres per second.
An open pipe (open at both ends) supports all integer harmonics with fundamental frequency v divided by 2L, while a pipe closed at one end supports only the odd harmonics with fundamental v divided by 4L. As a result, an open pipe of a given length sounds an octave higher than a closed pipe of the same length.
Yes, Waves is part of the NEET Physics syllabus and usually contributes a question or two each year, making it a reliable scoring chapter. The most frequently tested topics are standing waves in strings and organ pipes, beats, and the Doppler effect, so practising sign conventions in the Doppler formula and the closed-versus-open pipe distinction pays off.