NEET PhysicsNCERT Class 11Chapter 14

Waves: common doubts, answered

The questions students ask most often about Waves, each with a short answer. For the full chapter, read the Waves notes.

Waves carry energy, not matter

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Do the particles of the medium travel along with a wave?

No. Each particle only oscillates about its own mean position; it is the disturbance and its energy that travel. A cork on a pond bobs up and down as ripples pass but stays roughly where it is. A wave carries energy and momentum from one place to another without carrying the medium along.

Why does sound need a medium but light does not?

Sound is a mechanical wave: it travels by particles of a medium pushing on their neighbours, so without particles there is nothing to pass the disturbance along. Light is an electromagnetic wave made of changing electric and magnetic fields, which need no material medium and can cross empty space.

Transverse and longitudinal waves

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What is the difference between transverse and longitudinal waves?

In a transverse wave the particles oscillate perpendicular to the direction the wave travels, as on a plucked string. In a longitudinal wave they oscillate along the direction of travel, forming compressions and rarefactions, as in sound in air. Transverse mechanical waves need a medium that resists shearing, which is why they cannot travel through the bulk of a fluid.

Can sound travel as a transverse wave?

In gases and liquids, no; sound there is always longitudinal, because fluids have no shear modulus to support sideways oscillations. Solids can carry both kinds of mechanical wave, transverse and longitudinal, since they resist both shearing and compression. This is why both wave types travel through solid rock.

Displacement relation of a progressive wave

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How do you read wavelength and frequency from a wave equation?

Compare it with y(x, t) = a sin(kx − ωt + φ). The coefficient of x is the wave number k, and λ = 2π/k, not 1/k. The coefficient of t is ω, and the frequency is ν = ω/2π. The wave speed is v = ω/k. Mixing up k with 1/λ or ω with ν is the usual mistake.

How can you tell the direction a wave is moving from its equation?

If x and t appear with opposite signs, as in sin(kx − ωt), the wave moves in the positive x direction. If they have the same sign, as in sin(kx + ωt), it moves in the negative x direction. To see why, follow a crest: kx − ωt stays constant only if x increases as t increases.

What is the difference between wave velocity and particle velocity?

Wave velocity, v = λν, is how fast the disturbance moves through the medium and is constant for a given medium. Particle velocity is how fast an individual particle oscillates about its mean position, ∂y/∂t, which keeps changing with time. The two are entirely different quantities and are usually very different in size.

Wave speed on a stretched string

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What decides the speed of a wave on a string?

Only the tension T and the mass per unit length µ of the string: v = √(T/µ). The speed does not depend on the frequency of the source. A higher frequency gives a shorter wavelength on the same string, so that λν stays equal to the fixed speed. Tighter or lighter strings carry waves faster.

Speed of sound: Newton and Laplace

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Why was Newton's formula for the speed of sound wrong?

Newton assumed the compressions and rarefactions of sound happen isothermally, giving v = √(P/ρ), about 280 m/s in air, well below the measured value. Laplace pointed out the changes are too fast for heat to flow, so the process is adiabatic. That brings in γ, giving v = √(γP/ρ), which matches experiment.

Does pressure affect the speed of sound in air?

No, not at a fixed temperature. In v = √(γP/ρ), raising the pressure raises the density in the same ratio, so P/ρ stays constant. Temperature does change the speed, since warmer air at the same pressure is less dense; the speed of sound in a gas grows as the square root of absolute temperature.

Why does sound travel faster in solids than in air?

Because wave speed depends on the ratio of an elastic modulus to density, v = √(Y/ρ) in a bar. Solids are far more resistant to compression than gases, and this large modulus outweighs their greater density. So sound travels several kilometres per second in steel but only about 340 m/s in air.

Principle of superposition

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What is the principle of superposition of waves?

When two or more waves pass through the same point, the resulting displacement is the algebraic sum of the displacements each wave would produce alone. Afterwards, each wave carries on unchanged. Superposition explains interference, standing waves and beats, which all come from adding displacements of overlapping waves.

What happens when two waves meet in phase and out of phase?

If two identical waves meet in phase, their displacements add and the resultant amplitude is doubled, giving constructive interference. If they are exactly out of phase, by π, they cancel and the amplitude becomes zero, giving destructive interference. For any phase difference φ, the resultant amplitude is 2a cos(φ/2).

Reflection and standing waves

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What happens to a wave reflected from a rigid boundary?

It comes back inverted, with a phase change of π. A rigid end cannot move, so the incoming and reflected waves must add to zero displacement there, which requires the reflected pulse to be upside down. At an open or free boundary, the wave reflects without inversion, as the end is free to move.

What is the distance between two consecutive nodes in a standing wave?

It is λ/2, half a wavelength, not a full wavelength. The distance between a node and the nearest antinode is λ/4. A standing wave does not travel: nodes stay permanently at rest and antinodes oscillate with the largest amplitude, so energy is not carried along the medium.

What is the difference between a standing wave and a travelling wave?

A travelling wave moves through the medium, and every particle oscillates with the same amplitude, one after another. A standing wave forms when two identical waves travel in opposite directions; its pattern stays in place, with fixed nodes and antinodes, and the amplitude varies from point to point as 2a sin kx.

Harmonics of strings and pipes

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Why does a closed pipe produce only odd harmonics?

A pipe closed at one end must have a node at the closed end and an antinode at the open end. The pipe's length must then be an odd number of quarter wavelengths, so the allowed frequencies are (n + ½)v/2L: v/4L, 3v/4L, 5v/4L and so on. The even multiples cannot fit these boundary conditions.

What are the harmonics of a string fixed at both ends?

A string fixed at both ends must have a node at each end, so its length must be a whole number of half wavelengths. This gives frequencies ν = nv/2L, with n = 1, 2, 3, and so on. All harmonics are present, and the lowest, v/2L, is called the fundamental.

Beats

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What is the beat frequency?

It is the difference between the two frequencies, ν_beat = ν₁ − ν₂, not their sum. When two sounds of nearly equal frequency are heard together, their superposition makes the loudness rise and fall regularly. The number of loud swells per second equals this frequency difference.

How are beats used to tune a musical instrument?

A musician sounds the instrument together with a reference note and listens for beats. If beats are heard, the frequencies differ; the musician adjusts the string tension until the beats slow down and finally disappear, meaning the two frequencies match. This works because beats are easy to hear even when the frequency difference is tiny.

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