Periodic and oscillatory motion
Periodic motion repeats at regular intervals. Oscillatory motion is periodic motion about an equilibrium position. Time period T is the duration of one cycle; frequency ν = 1/T (Hz).
-- NCERT, p. 2Periodic motion is any motion that repeats at regular time intervals. The time for one complete cycle is the period (T); the number of cycles per second is the frequency (f = 1/T). NCERT Class 11 Physics Chapter 13, page 2 defines periodic motion and distinguishes it from oscillatory motion — every oscillation is periodic, but not every periodic motion is oscillatory (uniform circular motion is periodic but not oscillatory about a mean position).
Simple harmonic motion (SHM) is the simplest oscillatory motion. The displacement follows x(t) = A cos(ωt + φ), where ω = 2π/T. Two properties that trap aspirants repeatedly:
Trap 1 — Period is independent of amplitude. For an ideal spring (T = 2π√(m/k)) or a simple pendulum at small angles (T = 2π√(L/g)), doubling the amplitude does NOT change the period. The restoring force scales linearly with displacement, so larger swings produce proportionally larger restoring forces, keeping the timing unchanged. NEET exploits this by giving amplitude changes and asking for the new period — the answer is "period stays the same."
Trap 2 — Pendulum period is independent of bob mass. Because gravitational mass equals inertial mass, m cancels in the pendulum derivation. Questions that change the bob from iron to lead are testing whether you fall for a mass-dependence that does not exist.
Trap 3 — Closed-pipe harmonics are odd only. A pipe closed at one end supports only odd harmonics (f, 3f, 5f, …) because the closed end forces a displacement node. An open-open pipe supports all harmonics. Including even harmonics in a closed pipe is a common negative-marking error.
Watch out: these three traps appear in straightforward "what changes?" questions. The calculation is trivial — the conceptual clarity is what earns the mark.
Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.
A simple pendulum has a period of 2 s. If the bob mass is doubled while keeping the string length unchanged, the new period is:
A mass-spring system oscillates with amplitude A and period T. If the amplitude is increased to 2A (same spring, same mass), the new period is:
Which of the following is NOT an example of periodic motion?
A pipe closed at one end has a fundamental frequency of 200 Hz. The frequency of its second overtone is:
In SHM, a particle is at the mean position. At this instant, its:
A spring of spring constant k = 200 N/m is attached to a block of mass 0.50 kg on a frictionless surface. The block is displaced 0.10 m from equilibrium and released. The period of oscillation is closest to:
A simple pendulum of length 1.0 m has period T. If the length is increased to 4.0 m (same location), the new period is:
An open-open pipe of length L has a fundamental frequency f₀. A closed-end pipe of the same length L has a fundamental frequency f_c. The ratio f₀/f_c is:
Given
A spring extends by 0.050 m when a force of 10 N is applied. A block of mass 2.0 kg is attached to the spring on a frictionless horizontal surface and set into oscillation.
Required
Period of oscillation T.
Concept
First find the spring constant k from Hooke's law (F = kx), then use the mass-spring period formula T = 2π√(m/k). This is a two-step problem: derive k, then compute T.
Formula
- k = F/x - T = 2π√(m/k)
Substitution
- k = 10 N / 0.050 m = 200 N/m - T = 2π√(2.0 kg / 200 N/m)
Calculation
- m/k = 2.0/200 = 0.010 s² - √(0.010) = 0.100 s - T = 2π × 0.100 = 0.628 s Note on exact values: 2 and π are exact (counting integer and mathematical constant respectively). They do not limit significant figures. The answer precision is governed by the given data (2 significant figures).
Final answer
T ≈ 0.63 s
Common trap
A tempting wrong answer is to include the amplitude of oscillation in the period formula. Some aspirants try to use the 0.050 m extension as the amplitude and factor it into T. The period T = 2π√(m/k) has no amplitude dependence — doubling the pull-back does not change T.
Similar NEET-style question
A spring requires a force of 5.0 N to compress it by 0.025 m. If a 0.80 kg block is attached and released from the compressed position, find the oscillation period. (Answer: T = 2π√(0.80/200) ≈ 0.40 s.) ---
Periodic motion repeats at regular intervals. Oscillatory motion is periodic motion about an equilibrium position. Time period T is the duration of one cycle; frequency ν = 1/T (Hz).
-- 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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