Frequencies of standing waves: ν_n = n v / (2L) for n = 1, 2, 3, ... ν_1 is the fundamental (first harmonic); ν_2 = 2ν_1 is the second harmonic, etc.
-- NCERT, p. 12Standing Waves Strings Pipes
Lesson
The high-frequency trap in standing waves on strings and pipes is confusing which systems allow all harmonics and which allow only odd ones. A closed-end pipe supports only odd harmonics — yet students routinely plug in even harmonic numbers and lose marks.
Standing waves on a string fixed at both ends. When a transverse wave reflects at both fixed ends, superposition produces standing waves. Both ends are displacement nodes. The allowed frequencies are f_n = nv/(2L), where n = 1, 2, 3, … and v is the wave speed on the string (NCERT Class 11 Physics Chapter 14, page 12). All harmonics — fundamental, second, third, and so on — are present.
Standing waves in an open-open pipe. Both ends are displacement antinodes (pressure nodes). The formula is identical to the string: f_n = nv/(2L), with v now being the speed of sound. All harmonics are present (NCERT Class 11 Physics Chapter 14, page 13).
Standing waves in a closed-end pipe. One end is a displacement node (closed) and the other is a displacement antinode (open). The boundary asymmetry forces only odd harmonics: f_n = (2n−1)v/(4L), giving frequencies f, 3f, 5f, … (NCERT Class 11 Physics Chapter 14, page 13). Even harmonics (2f, 4f, …) are physically impossible in this geometry.
Why the closed pipe is different. The closed end demands a node and the open end demands an antinode. Fitting a standing wave between a node and the nearest antinode requires an odd number of quarter-wavelengths. That constraint eliminates every even harmonic.
The trap on paper. When a question says "pipe closed at one end," students who default to f_n = nv/(2L) — the string/open-pipe formula — will include forbidden even harmonics and pick a wrong option. Read the boundary condition first, then choose the formula.
Practice MCQs
Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.
A string fixed at both ends has a fundamental frequency of 200 Hz. What is the frequency of its third harmonic?
Which harmonics are present in a pipe closed at one end?
A pipe open at both ends has a fundamental frequency f. If one end is now closed (pipe length unchanged), the new fundamental frequency is:
The second overtone of an open-open pipe has a frequency of 900 Hz. What is the fundamental frequency of this pipe?
The second overtone of a pipe closed at one end has a frequency of 1250 Hz. What is the fundamental frequency?
A string of length 1.0 m is fixed at both ends and vibrates in its fundamental mode. The positions of nodes are at:
An open-open pipe of length L and a closed-end pipe of length L have the same speed of sound. The ratio of the fundamental frequency of the open pipe to that of the closed pipe is:
A closed-end pipe resonates at frequencies 850 Hz and 1190 Hz with no resonant frequency between them. What is the fundamental frequency of the pipe?
Quick recall before you leave
Worked Example
Pattern: Open-open vs closed-end pipe harmonic comparison (based on NEET pattern: compare frequency ratios across pipe types).
- 1
Given
An organ pipe open at both ends has a fundamental frequency of 480 Hz. The speed of sound is 340 m/s.
- 2
Required
(a) Find the length of the pipe. (b) If one end is now closed, find the fundamental frequency and the frequency of the 2nd overtone.
- 3
Concept
Open-open pipe: all harmonics, f_n = nv/(2L). Closed-end pipe: only odd harmonics, f_n = (2n−1)v/(4L). Closing one end changes the boundary condition from antinode-antinode to node-antinode.
- 4
Formula
Open pipe fundamental: f₁ = v/(2L) → L = v/(2f₁) Closed pipe fundamental: f₁' = v/(4L) Closed pipe 2nd overtone = 5th harmonic: f = 5v/(4L)
- 5
Substitution
L = 340/(2 × 480) = 340/960 f₁' = 340/(4 × 0.354) 2nd overtone = 5 × 340/(4 × 0.354)
- 6
Calculation
L = 340/960 ≈ 0.354 m f₁' = 340/(4 × 0.354) = 340/1.417 ≈ 240 Hz 2nd overtone of closed pipe = 5 × 240 = 1200 Hz **Note on exact values:** 480, 340, and the integer multipliers (2, 4, 5) are given or exact values — they do not limit significant figures. The division 340/960 is carried to three significant figures consistent with the input data.
- 7
Final answer
(a) L ≈ 0.354 m (about 35.4 cm) (b) Closed-pipe fundamental = 240 Hz; 2nd overtone = 1200 Hz Cross-check: 240 Hz is exactly half of 480 Hz, consistent with closing one end halving the fundamental. The 2nd overtone (5th harmonic) of the closed pipe at 1200 Hz is an odd multiple of 240 Hz. Both checks confirm the result.
- 8
Common trap
Using f_n = nv/(2L) for the closed pipe gives the 2nd overtone as 3 × 480 = 1440 Hz (the open pipe's 3rd harmonic), which is wrong. The closed pipe's 2nd overtone is the 5th harmonic at (2×3−1)v/(4L) = 5f₁', not 3f₁. Always check whether the pipe is open or closed before selecting the formula.
- 9
Similar NEET-style question
A pipe closed at one end has a fundamental frequency of 150 Hz. An open pipe of the same length is placed nearby. What is the fundamental frequency of the open pipe, and which is the lowest harmonic of the open pipe that matches a resonant frequency of the closed pipe? *Hint:* The open pipe's fundamental is 2 × 150 = 300 Hz. Its harmonics are 300, 600, 900, 1200, … Hz. The closed pipe's harmonics are 150, 450, 750, 1050, … Hz. Find the first common frequency. ---
Before solving, remember these
Standing waves in pipes
Open at both ends: ν_n = n v/(2L), all harmonics present. Closed at one end: ν_n = (2n-1) v/(4L), only odd harmonics.
-- NCERT, p. 13Formulas
10 formulas — click to collapse
Beat frequency
When 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 |
Valid when
- Linear superposition
- f1, f2 close in value
Period of simple pendulum (small angle)
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 |
Valid when
- Small angular amplitude (typically <15°)
- Massless string
- Point bob
SHM displacement
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 |
Valid when
- Restoring force linear (F = -kx)
- No damping
Total energy in SHM
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 |
Valid when
- Conservative SHM (no damping)
- Elastic regime
Period of mass-spring oscillator
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 |
Valid when
- Hooke's law spring
- No damping
- Small enough amplitude to stay in elastic regime
Standing wave in closed-end pipe
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 |
Valid when
- Closed at one end (open at other)
- End correction neglected
Standing wave in open-open pipe
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 |
Valid when
- Open at both ends
- End correction neglected
Standing wave frequencies on fixed-fixed string
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 | - |
Valid when
- String fixed at both ends
- Wave speed v as defined above
Speed of sound in gas (Newton-Laplace)
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 |
Valid when
- Ideal gas
- Adiabatic compression/expansion of sound waves
Wave speed on string
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 |
Valid when
- Stretched uniform string
- Small amplitude
Exam Traps & Common Mistakes
These are the exact patterns that cause wrong answers in NEET. Each trap includes when it triggers and how to avoid it.
6 items — click to collapse
Category: Overthinking
Student writes T as depending on bob mass. Simple pendulum T = 2π√(L/g); independent of m.
When it triggers
Question changes pendulum bob mass and asks for new period.
How to avoid
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.
When it triggers
Question gives changes in amplitude and asks for new period.
How to avoid
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, ...).
When it triggers
Question describes pipe closed at one end (e.g. resonance tube).
How to avoid
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
Correction
Simple pendulum T = 2π√(L/g) — independent of mass. Equivalence of inertial and gravitational mass cancels m.
Root cause: concept gap
Correction
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
Correction
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.
Past Year Questions
11 questions from NEET 2020, 2021, 2022, 2023, 2024, 2025. Answers verified against NTA official keys. — click to collapse
How NEET usually asks this
6 recurring patterns from past papers — click to collapse
Two strings/forks slightly out of tune produce beats; find one frequency given the other and beat frequency.
Common distractors
treats beat as sum
Adds frequencies instead of subtracting
Given pendulum length and g, find T. Or given mass change, observe T unchanged.
Common distractors
expects mass dependence
Assumes T depends on bob mass
Open-open pipe (all harmonics) vs closed-end pipe (odd only). Compare frequency ratios.
Common distractors
treats closed pipe like open
Includes even harmonics in closed pipe
Phase between displacement, velocity, acceleration in SHM. v leads x by π/2; a leads x by π.
Common distractors
uses pi 2 instead of pi
Confuses v-x phase with a-x phase
Given spring extension/compression with given force, find k, then find period when given mass m. T = 2*pi*sqrt(m/k).
Common distractors
forgets 2pi factor
Drops 2*pi
uses amplitude in period
Believes T depends on amplitude
Given tension change, find new wave speed on string. v ∝ sqrt(T).
Common distractors
uses linear tension scaling
Treats v ∝ T not sqrt(T)
Sources
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