Wave motion
A disturbance that propagates through a medium (or vacuum for EM waves) carrying energy and momentum without bulk transport of matter. Characterised by wavelength λ, frequency ν, period T, speed v.
-- NCERT, p. 2Wave motion is the transfer of energy and momentum through a medium (or vacuum, for electromagnetic waves) without bulk transfer of matter. NCERT Class 11 Physics Chapter 14, page 2 defines a wave as a disturbance that propagates through space and time, usually with a transfer of energy.
The trap NEET exploits: Students conflate the motion of the medium's particles with the motion of the wave itself. In a transverse wave on a string, particles move perpendicular to the wave's propagation direction. In a longitudinal wave (sound in air), particles oscillate parallel to propagation. The wave speed depends on medium properties — not on particle speed or amplitude.
Two key wave-speed relations:
For a transverse wave on a stretched string: v = √(T/μ), where T is tension and μ is linear mass density (NCERT Class 11 Physics Chapter 14, page 4). Speed depends on tension and mass distribution — not on frequency or amplitude.
For sound in a gas (longitudinal wave): v = √(γP/ρ), the Newton-Laplace formula (NCERT Class 11 Physics Chapter 14, page 5). Laplace's adiabatic correction fixed Newton's isothermal estimate, which underestimated the speed of sound by about 16%.
Common confusion: Changing frequency does NOT change wave speed in a given medium. The relation v = fλ means that if f changes (different source), λ adjusts — v stays fixed by the medium. Students who treat v as dependent on f lose marks on NEET problems that alter source frequency and ask for the new wavelength.
Watch-out: When tension on a string is quadrupled, wave speed doubles (v ∝ √T), not quadruples. The square-root relationship is a high-frequency distractor in NEET options.
Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.
In a transverse wave on a string, the particles of the medium move:
Which of the following correctly describes longitudinal waves?
The speed of a transverse wave on a string is v. If the tension in the string is increased to four times its original value while keeping the linear mass density unchanged, the new wave speed is:
A wave of frequency 200 Hz travels through a medium with a speed of 400 m/s. If the frequency of the source is changed to 400 Hz, the wave speed in the same medium becomes:
A wave travelling along a string is described by y(x,t) = 0.005 sin(80.0x − 3.0t), where x is in metres and t in seconds. The wavelength of the wave is:
Newton's formula for the speed of sound in air gave a value about 16% lower than the experimental value. Laplace corrected this by assuming sound propagation is:
A transverse wave on a string has speed v₁ when the tension is T₁. A second string has twice the linear mass density but is under the same tension T₁. The wave speed on the second string is:
A wave pulse is travelling along a string. Which of the following statements is correct?
Given
A transverse wave travels on a wire of length 1.0 m with a linear mass density μ = 4.0 × 10⁻³ kg/m. The wire is under a tension of 64 N. The wire is then tightened so that the tension becomes 100 N.
Required
Find the wave speed (a) at the original tension and (b) at the new tension.
Concept
Wave speed on a string depends on tension and linear mass density: v = √(T/μ). Speed is proportional to √T when μ is constant (NCERT Class 11 Physics Chapter 14, page 4).
Formula
v = √(T/μ)
Substitution
(a) v₁ = √(64 / 4.0 × 10⁻³) = √(16000) m/s (b) v₂ = √(100 / 4.0 × 10⁻³) = √(25000) m/s
Calculation
(a) √(16000) = √(16 × 1000) = 4√1000 = 4 × 31.62 ≈ 126.5 m/s (b) √(25000) = √(25 × 1000) = 5√1000 = 5 × 31.62 ≈ 158.1 m/s **Note on exact values:** The tension values 64 N and 100 N, and the linear mass density 4.0 × 10⁻³ kg/m, are given data (treated as exact for this problem). The integer factors (4 and 5) extracted from the square roots are exact counting numbers and do not affect significant-figure counts.
Final answer
(a) v₁ ≈ 1.26 × 10² m/s (b) v₂ ≈ 1.58 × 10² m/s Ratio check: v₂/v₁ = √(100/64) = √(25/16) = 5/4 = 1.25. Indeed, 158.1/126.5 ≈ 1.25. ✓
Common trap
Treating v ∝ T (linear) instead of v ∝ √T. With linear scaling, a student would get v₂ = v₁ × (100/64) = 1.5625 × v₁ ≈ 197.7 m/s — significantly overshooting the correct value. Always check: is the relationship linear or square-root?
Similar NEET-style question
"A wave on a string has speed 50 m/s when the tension is T. If the tension is increased to 9T without changing the string, what is the new wave speed?" Answer: v' = √(9T/μ) = 3√(T/μ) = 3 × 50 = 150 m/s. ---
A disturbance that propagates through a medium (or vacuum for EM waves) carrying energy and momentum without bulk transport of matter. Characterised by wavelength λ, frequency ν, period T, speed v.
-- NCERT, p. 2When two waves of nearly equal frequencies superpose, amplitude oscillates at the difference frequency.
| Symbol | Quantity | SI Unit |
|---|---|---|
| f_beat | beat frequency | Hz |
| f1, f2 | superposed frequencies | Hz |
Period of simple pendulum of length L. Holds for small amplitudes (sin theta ~ theta).
| Symbol | Quantity | SI Unit |
|---|---|---|
| T | period | s |
| L | pendulum length | m |
| g | gravity | m/s^2 |
Displacement in simple harmonic motion. Velocity = -A*omega*sin(omega*t+phi); a = -omega^2 * x.
| Symbol | Quantity | SI Unit |
|---|---|---|
| A | amplitude | m |
| omega | angular frequency | rad/s |
| phi | phase | rad |
| T | period | s |
| f | frequency | Hz |
Total mechanical energy is constant. Oscillates between KE (max at x=0) and PE (max at x=±A).
| Symbol | Quantity | SI Unit |
|---|---|---|
| E | total energy | J |
| k | spring constant | N/m |
| A | amplitude | m |
| m | mass | kg |
| omega | angular frequency | rad/s |
Period of horizontal spring with mass m, spring constant k. Independent of amplitude.
| Symbol | Quantity | SI Unit |
|---|---|---|
| T | period | s |
| m | mass | kg |
| k | spring constant | N/m |
Pipe closed at one end has only odd harmonics: f, 3f, 5f, ...
| Symbol | Quantity | SI Unit |
|---|---|---|
| f_n | n-th harmonic | Hz |
| v | sound speed | m/s |
| L | pipe length | m |
Pipe open at both ends has all harmonics. Same formula as string.
| Symbol | Quantity | SI Unit |
|---|---|---|
| f_n | n-th harmonic | Hz |
| v | sound speed | m/s |
| L | pipe length | m |
Allowed frequencies on string fixed at both ends. n=1 fundamental; harmonics 2f, 3f, ...
| Symbol | Quantity | SI Unit |
|---|---|---|
| f_n | n-th harmonic | Hz |
| v | wave speed on string | m/s |
| L | string length | m |
| n | harmonic number | - |
Speed of sound in gas. Adiabatic index gamma, pressure P, density rho. Increases with sqrt(T).
| Symbol | Quantity | SI Unit |
|---|---|---|
| v | speed of sound | m/s |
| gamma | adiabatic index | - |
| P | pressure | Pa |
| rho | density | kg/m^3 |
Speed of transverse wave on string under tension T, linear mass density mu.
| Symbol | Quantity | SI Unit |
|---|---|---|
| v | wave speed | m/s |
| T | tension | N |
| mu | linear mass density | kg/m |
These are the exact patterns that cause wrong answers in NEET. Each trap includes when it triggers and how to avoid it.
Category: Overthinking
Student writes T as depending on bob mass. Simple pendulum T = 2π√(L/g); independent of m.
Question changes pendulum bob mass and asks for new period.
Mass cancels in derivation (gravitational mass = inertial mass). Mass changes the bob's KE and PE proportionally; period unaffected.
Category: Overthinking
Student claims SHM period depends on amplitude. For ideal SHM (Hooke's law spring or simple pendulum at small angle), period is INDEPENDENT of amplitude.
Question gives changes in amplitude and asks for new period.
T = 2π√(m/k) (spring) or 2π√(L/g) (pendulum, small angle) — neither depends on A. Only at large pendulum angles does T pick up a small amplitude correction.
Category: Similar Terms
Student includes even harmonics in a closed-end pipe. Closed pipe has only ODD harmonics (f, 3f, 5f, ...).
Question describes pipe closed at one end (e.g. resonance tube).
Open both ends: all harmonics, f_n = nv/(2L). Closed one end: odd only, f_n = (2n-1)v/(4L). Fundamental of closed pipe is HALF that of open pipe of same L.
Root cause: concept gap
Simple pendulum T = 2π√(L/g) — independent of mass. Equivalence of inertial and gravitational mass cancels m.
Root cause: concept gap
Ideal SHM: T = 2π√(m/k) (spring) or 2π√(L/g) (pendulum, small angle) — no amplitude dependence. Doubling amplitude does not change period.
Root cause: concept gap
Closed-end pipe has only ODD harmonics (f, 3f, 5f, ...). Open-both-ends pipe has all (f, 2f, 3f, ...). Reason: closed end has displacement node and pressure antinode.
treats beat as sum
Adds frequencies instead of subtracting
expects mass dependence
Assumes T depends on bob mass
treats closed pipe like open
Includes even harmonics in closed pipe
uses pi 2 instead of pi
Confuses v-x phase with a-x phase
forgets 2pi factor
Drops 2*pi
uses amplitude in period
Believes T depends on amplitude
uses linear tension scaling
Treats v ∝ T not sqrt(T)
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