Time period of spring
For mass m attached to spring of force constant k: T = 2π √(m/k). Independent of amplitude. ω = √(k/m).
-- NCERT, p. 5A block on a spring is pulled aside and released. It oscillates. Why? Because the spring exerts a restoring force — a force that always points back toward the equilibrium position. This force is what makes simple harmonic motion possible.
For an ideal spring obeying Hooke's law, the restoring force is F = −kx, where k is the force constant (also called spring constant) and x is displacement from equilibrium. The negative sign encodes the "restoring" nature: displace right, force pulls left; displace left, force pushes right. The force constant k has units N/m and measures stiffness — a larger k means a stiffer spring and a stronger pull back to equilibrium (NCERT Class 11 Physics, Chapter 13, page 5).
Connect this to the period of oscillation: T = 2π√(m/k). A stiffer spring (larger k) gives a shorter period — the system snaps back faster. A heavier mass (larger m) gives a longer period — more inertia to overcome.
The trap that costs marks: students believe that changing the amplitude changes the period. It does not. The formula T = 2π√(m/k) contains neither amplitude A nor the initial displacement. Double the amplitude and the block travels farther, but it also moves faster (larger restoring force at larger displacement). These effects cancel exactly, leaving the period unchanged. This is a high-frequency confusion in NEET — when you see a problem that changes amplitude and asks for the new period, the answer is: the period stays the same.
Watch out: the force constant k is a property of the spring, not the mass. If a problem says "a 2.0 N/cm spring," convert to SI (200 N/m) before substituting into T = 2π√(m/k).
Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.
The SI unit of force constant (spring constant) is:
In Hooke's law F = −kx, the negative sign indicates that the force:
A spring has a force constant of 400 N/m. This means that:
A spring stretches by 5.0 cm when a force of 10 N is applied. The force constant of the spring is:
A body of mass 0.50 kg is attached to a spring of force constant 200 N/m and set into oscillation. The period of oscillation is closest to:
A mass-spring system oscillates with amplitude A and period T. If the amplitude is doubled to 2A while everything else remains unchanged, the new period is:
A spring extends by 4.0 cm when a force of 8.0 N is applied. A block of mass 0.80 kg is now attached to this spring and set into oscillation. The period of oscillation is closest to:
Two springs have force constants k₁ = 100 N/m and k₂ = 300 N/m. They are connected in parallel and a 1.0 kg block is attached. The period of oscillation of the block is closest to:
Given
- Applied force: F = 10.0 N - Compression: x = 5.0 cm = 5.0 × 10⁻² m - Mass of block: m = 2.0 kg
Required
Period of oscillation T.
Concept
The spring obeys Hooke's law (F = kx), so we first find k from the static load data. Then we use T = 2π√(m/k) to find the period of SHM.
Formula
k = F/x (from Hooke's law) T = 2π√(m/k) (period of mass-spring oscillator)
Substitution
k = 10.0 N / (5.0 × 10⁻² m) T = 2π√(2.0 kg / k)
Calculation
k = 10.0 / 0.050 = 200 N/m m/k = 2.0 / 200 = 1.0 × 10⁻² s² √(1.0 × 10⁻²) = 0.10 s T = 2π × 0.10 = 0.6283 s **Exact constants note:** The factors 2 and π are exact mathematical constants. They do not limit significant figures. The answer's precision is governed by the given data (2 significant figures).
Final answer
T ≈ 0.63 s (Rounded to 2 significant figures, matching the precision of the given data.)
Common trap
The amplitude of oscillation (5.0 cm initial compression) does not appear in the period formula. If the problem changes the amplitude — say the spring is now compressed by 10 cm — the period remains 0.63 s. This is the amplitude-independence trap documented in trap: period amplitude dependence: students who include amplitude in their period calculation get a wrong answer.
Similar NEET-style question
A spring of force constant 800 N/m supports a 0.50 kg mass. The mass is pulled down 3.0 cm and released. What is the time period? (Answer: T = 2π√(0.50/800) = 2π × 0.025 = 0.157 s ≈ 0.16 s. The 3.0 cm pull-down is irrelevant to the period.) ---
For mass m attached to spring of force constant k: T = 2π √(m/k). Independent of amplitude. ω = √(k/m).
-- 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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