Speed of wave on string
v = √(T/μ), where T is tension and μ is linear mass density (mass per unit length). Doubling tension increases speed by √2.
-- NCERT, p. 4The speed of a travelling wave depends on the medium, not on the source. Two formulas govern this topic at the NEET level, and one common error connects them.
Transverse wave on a string. The speed is v = √(T/μ), where T is the tension in the string and μ is the linear mass density (mass per unit length). This is derived from Newton's second law applied to a small element of the string (NCERT Class 11 Physics Chapter 14, page 4). The key relationship: v scales as √T, not as T. Doubling the tension increases speed by a factor of √2, not 2. This is a high-frequency distractor in NEET — students who treat v as directly proportional to T pick the wrong option.
Speed of sound in a gas. The Newton-Laplace formula gives v = √(γP/ρ), where γ is the adiabatic index, P the gas pressure, and ρ the density (NCERT Class 11 Physics Chapter 14, page 5). Newton's original formula used isothermal bulk modulus (B = P), predicting a value about 15% below the measured speed of sound in air. Laplace corrected it by recognising that sound compressions are adiabatic, replacing P with γP.
The connection that trips students: both formulas have the form v = √(elastic property / inertial property). For the string, the elastic property is tension and the inertial property is linear mass density. For the gas, the elastic property is γP (adiabatic bulk modulus) and the inertial property is density ρ.
Watch out: wave speed on a string is independent of frequency and wavelength — those are set by the source. Changing tension changes v, which then changes the wavelength for a given frequency (v = fλ), but does not change the frequency itself.
Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.
The speed of a transverse wave on a stretched string depends on:
Laplace corrected Newton's formula for the speed of sound in air by replacing the isothermal process with:
In the Newton-Laplace formula v = √(γP/ρ), what does γ represent?
The tension in a stretched string is increased to 4 times its original value while the linear mass density remains unchanged. The wave speed becomes:
A transverse wave travels on a string with speed 40 m/s when the tension is 100 N. If the tension is reduced to 25 N, what is the new wave speed?
The speed of sound in oxygen at a given temperature is v. The speed of sound in hydrogen at the same temperature and pressure is (assume both are diatomic):
A string of length 2.0 m has a total mass of 20 g. It is stretched with a tension of 80 N. A transverse wave of frequency 200 Hz travels along the string. The wavelength is:
The speed of sound in air at 0 °C is 332 m/s. If the temperature is raised to 546 °C, the speed of sound becomes approximately:
Pattern: Wave speed on a string changes when tension changes (based on PYQ pattern NEET pattern: wave speed tension — observed NEET 2022).
Given
- v₁ = 60 m/s - T₁ = 36 N - T₂ = 144 N - μ unchanged
Required
- v₂ = ?
Concept
Wave speed on a string depends on tension and linear mass density: v = √(T/μ). When μ is constant, speed scales as the square root of tension.
Formula
v₂/v₁ = √(T₂/T₁)
Substitution
v₂/v₁ = √(144/36) = √4
Calculation
v₂/v₁ = 2 v₂ = 2 × 60 = 120 m/s Note on exact values: 36 N, 144 N, and 60 m/s are problem-defined exact values. The integers 2 and 4 are exact. These do not limit significant figures.
Final answer
v₂ = 120 m/s
Common trap
Treating v as directly proportional to T (linear scaling) would give v₂ = 60 × (144/36) = 60 × 4 = 240 m/s — exactly double the correct answer. The square-root dependence is the key: v ∝ √T.
Similar NEET-style question
A wave travels at speed v on a wire under tension T. The wire is replaced by one with the same material but double the diameter (hence 4× the cross-sectional area and 4× the linear mass density). If tension remains the same, what is the new speed? (Answer: v/2, since v = √(T/μ) and μ → 4μ gives v → v/√4 = v/2.) ---
v = √(T/μ), where T is tension and μ is linear mass density (mass per unit length). Doubling tension increases speed by √2.
-- NCERT, p. 4v = √(γ P/ρ) (Newton-Laplace formula). For air at STP: v ≈ 343 m/s. Increases with temperature: v ∝ √T.
-- NCERT, p. 5When 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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