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Waves Notes for NEET and JEE Main 2027: Key Points and PDF

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Waves is Chapter 14 of NCERT Class 11 Physics (Part II) and the second half of Unit 10, Oscillations and Waves, in both the NEET UG and JEE Main syllabus. These notes cover transverse and longitudinal waves, the progressive wave equation, wave speed, Laplace’s correction, superposition, reflection, standing waves in strings and pipes, and beats, with a free PDF.

Waves Notes for NEET and JEE Main

Section-wise key points from NCERT Chapter 14, formula tables, high-yield facts and common mistakes for 2027 revision.

Waves at a Glance

ItemDetails
Syllabus unitUnit 10: Oscillations and Waves (same unit number in NEET UG and JEE Main)
Exams that cover itNEET UG and JEE Main Paper 1 (B.E./B.Tech.)
NCERT textbookPhysics Part II, Class 11, Chapter 14 (rationalised book)
Other chapter in the unitOscillations (Chapter 13)
Syllabus topicsWave motion; longitudinal and transverse waves; speed of the travelling wave; displacement relation for a progressive wave; principle of superposition; reflection of waves; standing waves in strings and organ pipes; fundamental mode and harmonics; beats
Experimental skills (Unit 20)Speed of sound in air at room temperature using a resonance tube
Official chapterNCERT Chapter 14
Notes PDFView PDF

The topic list follows the NEET UG 2026 syllabus released by the National Medical Commission (NMC) on 22 December 2025 and the JEE Main 2026 syllabus published by the National Testing Agency (NTA). Both stay the reference until the 2027 syllabi are out. The full lists are on the NEET syllabus and JEE Main syllabus pages. The Doppler effect is not in the rationalised NCERT chapter or in either syllabus, so it is not covered here.

Transverse and Longitudinal Waves

A mechanical wave carries energy, not matter, through a material medium; elastic forces couple neighbouring oscillating parts of the medium.

FeatureTransverse waveLongitudinal wave
Particle motionPerpendicular to the direction of propagationAlong the direction of propagation
Elastic property neededShear modulusBulk modulus
MediaSolids and strings (not in fluids)Solids, liquids and gases
ExampleWave on a stretched stringSound in air (compressions and rarefactions)
  • Mechanical waves need a medium and are governed by Newton’s laws; electromagnetic waves need no medium.
  • A wave is not motion of matter as a whole: wind moves air from place to place, while a sound wave only compresses and rarefies layers of air.
  • A progressive (travelling) wave moves from one point of the medium to another.

Displacement Relation for a Progressive Wave

A sinusoidal wave travelling in the positive x direction is y(x, t) = a sin(kx − ωt + φ); for the negative x direction the phase is kx + ωt + φ.

TermSymbol and relationMeaning
AmplitudeaMaximum displacement of an element of the medium
Phasekx − ωt + φDescribes the state of motion at x and t
WavelengthλDistance between two consecutive points in the same phase
Angular wave numberk = 2π/λSI unit rad m⁻¹
PeriodT = 2π/ωTime for one complete oscillation of an element
Frequencyν = 1/T = ω/2πOscillations per second (Hz)
  • In a harmonic progressive wave all particles have the same amplitude but different phases at a given instant.

Speed of a Travelling Wave

Wave speed is v = λ/T = λν = ω/k, and it is set by the elastic and inertial properties of the medium, not by the source’s velocity.

WaveSpeed formulaNotes
Transverse wave on a stringv = √(T/µ)T = tension, µ = linear mass density; independent of frequency
Longitudinal wave in a fluidv = √(B/ρ)B = bulk modulus, ρ = density
Longitudinal wave in a solid barv = √(Y/ρ)Y = Young’s modulus
Sound in a gas: Newton’s formulav = √(P/ρ)Assumes isothermal changes; gives about 280 m s⁻¹ in air at STP
Sound in a gas: Laplace correctionv = √(γP/ρ)Changes are adiabatic; with γ = 7/5 gives 331.3 m s⁻¹ in air at STP
  • Newton’s value is about 15% lower than the measured 331 m s⁻¹, because sound compressions are too fast for heat to flow; the process is adiabatic, not isothermal.
  • Sound travels faster in solids and liquids because their elastic moduli are much higher.
  • At a fixed temperature P/ρ is constant, so the speed of sound in a gas does not depend on pressure; it rises with temperature and with humidity.

Principle of Superposition and Interference

When waves overlap, the resultant displacement of each element is the algebraic sum of the displacements due to each wave: y = Σ f<sub>i</sub>(x − vt).

  • Wave pulses keep their identities after crossing each other.
  • Two waves of equal amplitude a and frequency travelling in the same direction with phase difference φ combine into y = 2a cos(φ/2) sin(kx − ωt + φ/2).
  • Resultant amplitude is 2a cos(φ/2).
  • Constructive interference: φ = 0 or an integral multiple of 2π (amplitude 2a). Destructive interference: φ = π (amplitude zero).

Reflection of Waves

A wave reflected at a rigid boundary returns with a phase reversal; at an open boundary it reflects without a phase change.

BoundaryReflected wave for y<sub>i</sub> = a sin(kx − ωt)Phase change
Rigid boundary or closed endy<sub>r</sub> = −a sin(kx + ωt)π (phase reversal)
Open boundaryy<sub>r</sub> = a sin(kx + ωt)None

Standing Waves and Normal Modes

Two identical waves travelling in opposite directions produce a standing wave, y(x, t) = [2a sin kx] cos ωt, with fixed nodes and antinodes.

  • Nodes: points of zero displacement; antinodes: points of maximum displacement.
  • Distance between consecutive nodes or consecutive antinodes = λ/2.
  • In a stationary wave, all particles between two nodes have the same phase but different amplitudes.
  • Each allowed frequency of a string or air column is a normal mode and a resonant frequency of the system.
SystemAllowed frequenciesFundamentalHarmonics present
String fixed at both ends (length L)ν = nv/2L, n = 1, 2, 3, …v/2LAll harmonics
Pipe closed at one endν = (n + ½)v/2L, n = 0, 1, 2, …v/4LOdd harmonics only
Pipe open at both endsν = nv/2L, n = 1, 2, 3, …v/2LAll harmonics (each end is an antinode)
  • The lowest frequency is the fundamental mode or first harmonic; the mode with n = 2 on a string is the second harmonic.
  • NCERT example: a 30.0 cm pipe open at both ends (v = 330 m s⁻¹) has a fundamental of 550 Hz, so a 1.1 kHz source excites its second harmonic; with one end closed it would not resonate, since only odd harmonics occur.

Beats

Beats are the periodic waxing and waning of loudness heard when two waves of slightly different frequencies and comparable amplitudes are superposed.

  • Beat frequency: ν<sub>beat</sub> = ν₁ − ν₂ (the difference of the two frequencies).
  • Musicians tune instruments against each other until no beats are heard.

Most-asked Facts for NEET and JEE Main: Waves

Revise these one-line facts from the NCERT chapter just before the exam.

  • v = λν = ω/k; k = 2π/λ; ω = 2πν.
  • Speed on a stretched string: v = √(T/µ).
  • Speed of sound in a gas: v = √(γP/ρ) (Laplace correction).
  • Newton’s isothermal formula gives about 280 m s⁻¹ for air at STP; Laplace’s gives 331.3 m s⁻¹.
  • Transverse waves need shear modulus; longitudinal waves need bulk modulus.
  • Reflection at a rigid end: phase change π; at an open end: no phase change.
  • Node to node distance = λ/2.
  • String fixed at both ends and pipe open at both ends: all harmonics, fundamental v/2L.
  • Pipe closed at one end: odd harmonics only, fundamental v/4L.
  • Beat frequency = ν₁ − ν₂.
  • A wave transfers energy, not matter.

Common Mistakes to Avoid

Watch for these mix-ups when you answer questions on this chapter.

  • Saying the speed of sound in air changes with pressure at constant temperature. P/ρ stays constant, so it does not.
  • Using Newton’s formula v = √(P/ρ) for sound in air. The correct one includes γ (Laplace correction).
  • Giving a closed pipe even harmonics. A pipe closed at one end has only odd harmonics.
  • Taking node-to-node spacing as λ. It is λ/2; node to adjacent antinode is λ/4.
  • Thinking wave speed depends on the source’s speed or on frequency. It depends on the medium.
  • Confusing particle velocity (∂y/∂t) with wave speed v.
  • Expecting transverse waves in the bulk of a gas or liquid. Fluids have no shear modulus, so they carry only longitudinal waves.

Download the AglaSem Class 11 Physics notes for Oscillations and Waves (key notes and important questions with answers) free: View PDF. The same PDF covers Oscillations. It also has older topics, such as the Doppler effect, that are not in the rationalised NCERT chapter.

Physics Notes for NEET and JEE Main: All Chapters

All chapters with key points and notes PDFs are on the Physics notes for NEET and JEE Main page.

Waves Notes for NEET and JEE Main FAQs

Which NCERT chapter is Waves?
It is Chapter 14 of the rationalised NCERT Class 11 Physics Part II textbook, the last chapter of the book. Oscillations (Chapter 13) comes before it in Unit 10, Oscillations and Waves.
Is Waves in the NEET 2027 and JEE Main 2027 syllabus?
It is part of Unit 10, Oscillations and Waves, in both the NEET UG 2026 syllabus (NMC, 22 December 2025) and the JEE Main 2026 syllabus (NTA). The 2027 syllabi are not out yet; check this page and the syllabus pages when they are released.
Is the Doppler effect in the NEET and JEE Main syllabus?
The Waves topics in the NEET UG 2026 and JEE Main 2026 syllabi end with standing waves, harmonics and beats, and the rationalised NCERT chapter has no Doppler effect section. Revise it only if a newer syllabus adds it back.
What is Laplace’s correction?
Newton assumed sound compressions are isothermal and got v = √(P/ρ), about 280 m s⁻¹ in air. Laplace showed they are adiabatic, so v = √(γP/ρ); with γ = 7/5 this gives 331.3 m s⁻¹, matching experiment.
Are these notes enough for Waves questions?
No. Read NCERT Chapter 14 fully, including the standing-wave and pipe examples, then solve numerical problems. Use these notes and the PDF for quick revision and practise previous year questions.
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