1. Chapter at a Glance
An oscillation is a to-and-fro motion about a mean position. The simplest and most important kind is simple harmonic motion (SHM), where the restoring force is proportional to displacement. Springs, pendulums, vibrating strings and AC circuits all follow the same mathematics. The chapter covers the SHM equation, velocity and acceleration, energy, spring and pendulum systems, and an introduction to damped and forced oscillations. JEE Main asks one question almost every year.
- Displacement, velocity, acceleration and phase in SHM.
- Kinetic and potential energy at a given displacement.
- Time period of spring systems (series/parallel) and pendulums (in lifts, on other planets).
- Time taken between two positions.
2. Simple Harmonic Motion
SHM happens when F = −kx, i.e. a = −ω²x. The solution is:
- A = amplitude, ω = angular frequency, T = 2π/ω, f = 1/T, (ωt + φ) = phase, φ = initial phase.
- Maximum speed vmax = Aω at the mean position; maximum acceleration amax = Aω² at the extreme positions.
- Velocity leads displacement by π/2; acceleration is π out of phase with displacement.
- SHM is the projection of uniform circular motion on a diameter.
3. Energy in SHM
- Total energy is constant; KE and PE interchange. They are equal at x = A/√2.
- KE and PE each oscillate with frequency 2f (period T/2).
- Average KE = average PE = E/2 over a cycle.
4. Spring and Pendulum Systems
| System | Time period |
|---|---|
| Mass on a spring | T = 2π√(m/k) |
| Springs in series | 1/k = 1/k₁ + 1/k₂ |
| Springs in parallel (or on both sides of a block) | k = k₁ + k₂ |
| Spring cut into n equal parts | each part has constant nk |
| Simple pendulum (small angle) | T = 2π√(l/g) |
| Pendulum in lift (acceleration a up/down) | T = 2π√(l/(g ± a)) |
| Liquid in U-tube (column length L) | T = 2π√(L/2g) |
| Floating body (submerged depth h) | T = 2π√(h/g) |
| Physical pendulum | T = 2π√(I/mgd) |
A pendulum with period exactly 2 s is a "seconds pendulum" (length ≈ 1 m on Earth). The period of a spring–mass system does not depend on g, so it is the same on the Moon or in a lift.
5. Damped and Forced Oscillations
- Damped oscillation: amplitude decreases with time because of friction or drag: A(t) = A₀e−bt/2m.
- Forced oscillation: a periodic driving force makes the system oscillate at the driver's frequency.
- Resonance: when the driving frequency equals the natural frequency, the amplitude becomes very large (limited only by damping). Examples: soldiers break step on bridges; tuning a radio.
6. Formula Master Table
| Quantity | Formula |
|---|---|
| Condition for SHM | a = −ω²x |
| Displacement | x = A sin(ωt + φ) |
| Velocity | v = ω√(A² − x²); vmax = Aω |
| Acceleration | amax = Aω² |
| Total energy | E = ½kA² |
| Spring | T = 2π√(m/k) |
| Pendulum | T = 2π√(l/geff) |
| Time from mean to A/2 | T/12 |
7. Mind Map
- a = −ω²x
- x, v, a and phase
- KE + PE = ½kA²
- Frequency 2f
- Springs (series/parallel)
- Pendulum, geff
- U-tube, floating body
- Decaying amplitude
- Forced, resonance
8. Tips and Tricks
- Use the phasor (reference circle) picture for time questions: mean → A/2 takes T/12, A/2 → A takes T/6.
- If two speeds v₁, v₂ at displacements x₁, x₂ are given: ω² = (v₁² − v₂²)/(x₂² − x₁²).
- In any accelerated frame, replace g by the effective g for a pendulum.
- A block between two springs attached to walls on either side: keff = k₁ + k₂.
- Using the pendulum formula for large angles (it is valid only for small angles).
- Thinking a spring–mass period changes on the Moon.
- Confusing angular frequency ω with frequency f (ω = 2πf).
9. Important One-liners
- In SHM, speed is maximum at the mean position and zero at the extremes.
- Acceleration is maximum at the extremes and zero at the mean position.
- The period of SHM does not depend on amplitude.
- A pendulum does not oscillate in a freely falling lift.
- Kinetic energy oscillates at twice the frequency of the motion.
- At resonance, the amplitude of a forced oscillation is maximum.
10. Solved Numericals: Average to Advanced
Five average-level and five advanced-level problems. Click to reveal each answer and its full working. Take g = 10 m s⁻² and π² ≈ 9.87 where needed.
Average level
A 0.5 kg mass is attached to a spring of constant 50 N m⁻¹. Find ω and the time period.
Show answer & solution
Concept: ω = √(k/m); T = 2π/ω.
- ω = √(50/0.5) = √100 = 10 rad s⁻¹.
- T = 2π/10 ≈ 0.628 s.
Answer: 10 rad s⁻¹; 0.628 s
A particle moves as x = 5 sin(2t + π/6) cm (t in s). Find its amplitude, period, maximum speed and maximum acceleration.
Show answer & solution
Concept: compare with x = A sin(ωt + φ).
- A = 5 cm; ω = 2 rad s⁻¹ ⇒ T = 2π/2 = π ≈ 3.14 s.
- vmax = Aω = 10 cm s⁻¹.
- amax = Aω² = 20 cm s⁻².
Answer: 5 cm; π s; 10 cm s⁻¹; 20 cm s⁻²
Find the length of a simple pendulum whose period is 2 s.
Show answer & solution
Concept: T = 2π√(l/g) ⇒ l = gT²/4π².
- l = 10 × 4/(4 × 9.87).
- ≈ 1.01 m.
Answer: about 1.0 m
For a particle in SHM of amplitude A, find (a) the ratio KE : PE and (b) the speed, when the displacement is A/2.
Show answer & solution
Concept: KE ∝ (A² − x²), PE ∝ x².
- PE ∝ A²/4; KE ∝ A² − A²/4 = 3A²/4.
- KE : PE = 3 : 1.
- v = ω√(A² − A²/4) = (√3/2)Aω ≈ 0.87 vmax.
Answer: 3 : 1; (√3/2)Aω
A 0.5 kg block on a spring (k = 50 N m⁻¹) oscillates with amplitude 0.1 m. Find its total energy and maximum speed.
Show answer & solution
Concept: E = ½kA²; at the mean position E is all kinetic.
- E = ½ × 50 × 0.01 = 0.25 J.
- ½ × 0.5 × vmax² = 0.25 ⇒ vmax = 1 m s⁻¹ (also Aω = 0.1 × 10).
Answer: 0.25 J; 1 m s⁻¹
Advanced level
Two identical springs, each 100 N m⁻¹, support the same mass, first in series and then in parallel. Find the effective spring constants and the ratio of the periods Tseries : Tparallel.
Show answer & solution
Concept: series 1/k = 1/k₁ + 1/k₂; parallel k = k₁ + k₂; T ∝ 1/√k.
- ks = 100 × 100/200 = 50 N m⁻¹.
- kp = 200 N m⁻¹.
- Ts/Tp = √(kp/ks) = √4 = 2.
Answer: 50 and 200 N m⁻¹; 2 : 1
A 1 m simple pendulum hangs in a lift. Find its period when the lift (a) is at rest, (b) accelerates upward at 2.5 m s⁻², (c) falls freely.
Show answer & solution
Concept: T = 2π√(l/geff), with geff = g + a (upward acceleration).
- (a) T = 2π√(1/10) ≈ 1.99 s.
- (b) geff = 12.5 m s⁻²: T = 2π√(1/12.5) ≈ 1.78 s.
- (c) geff = 0: the pendulum does not oscillate (T → ∞).
Answer: 1.99 s; 1.78 s; no oscillation
A particle executes SHM with period 12 s, starting from the mean position. Find the time it takes to reach (a) half the amplitude, (b) the extreme position from half the amplitude.
Show answer & solution
Concept: x = A sin(ωt), ω = 2π/T.
- (a) A/2 = A sin(ωt) ⇒ ωt = π/6 ⇒ t = (π/6)/(2π/12) = 1 s (= T/12).
- Time from mean to extreme = T/4 = 3 s.
- (b) From A/2 to A = 3 − 1 = 2 s (= T/6).
Answer: 1 s; 2 s
(a) A liquid column of total length 0.4 m oscillates in a U-tube. Find its period. (b) A block of mass 1 kg is fixed between two walls by springs of 100 N m⁻¹ and 300 N m⁻¹ on either side. Find its period.
Show answer & solution
Concept: (a) U-tube: restoring force = 2ρAgx for mass ρAL ⇒ T = 2π√(L/2g). (b) Both springs push back ⇒ k = k₁ + k₂.
- (a) T = 2π√(0.4/20) = 2π√0.02 ≈ 0.89 s.
- (b) k = 100 + 300 = 400 N m⁻¹.
- T = 2π√(1/400) = 2π/20 ≈ 0.314 s.
Answer: (a) about 0.89 s; (b) about 0.31 s
A particle in SHM has speed 3 cm s⁻¹ at 4 cm from the mean position and 4 cm s⁻¹ at 3 cm from it. Find the amplitude and period.
Show answer & solution
Concept: v² = ω²(A² − x²) at both points.
- 9 = ω²(A² − 16) and 16 = ω²(A² − 9).
- Subtract: 7 = ω²(16 − 9) = 7ω² ⇒ ω = 1 rad s⁻¹.
- Then 9 = A² − 16 ⇒ A² = 25 ⇒ A = 5 cm.
- T = 2π/ω = 2π ≈ 6.28 s.
Answer: 5 cm; 2π s
11. PYQ-pattern Questions with Solutions
These questions are original and modelled on concepts frequently tested in JEE Main.
In SHM, the acceleration is maximum:
- At the mean position
- At the extreme positions
- Midway
- Everywhere the same
Show solution
a = −ω²x is largest in magnitude when |x| = A.
Answer: (B)
A particle performs SHM with frequency f. Its kinetic energy varies with frequency:
- f/2
- f
- 2f
- 4f
Show solution
KE ∝ cos²(ωt) = (1 + cos 2ωt)/2, so it repeats at 2f.
Answer: (C)
A pendulum clock is taken to the Moon (gmoon = g/6). Its period becomes:
- T/6
- 6T
- √6 T
- T/√6
Show solution
T ∝ 1/√g, so T′ = T√6.
Answer: (C)
The phase difference between displacement and acceleration of a particle in SHM is:
- 0
- π/2
- π
- 3π/2
Show solution
a = −ω²x = ω²x sin(… + π): acceleration is always opposite to displacement.
Answer: (C)
A spring of constant 100 N m⁻¹ is cut into two equal halves. Find the spring constant (in N m⁻¹) of each half.
Show solution
k ∝ 1/length, so each half has 2 × 100 = 200 N m⁻¹.
Answer: 200
A particle moves as x = 4 cos(πt) m. Find its period in seconds.
Show solution
ω = π ⇒ T = 2π/π = 2 s.
Answer: 2
12. Quick Revision Summary
- SHM: a = −ω²x; x = A sin(ωt + φ); v = ω√(A² − x²).
- vmax = Aω; amax = Aω²; E = ½kA².
- Spring T = 2π√(m/k); series/parallel rules; cut spring stiffer.
- Pendulum T = 2π√(l/geff).
- Mean → A/2: T/12; A/2 → A: T/6.