Energy in SHM
KE(t) = ½ m ω² A² sin²(ωt+φ); PE(t) = ½ k x² = ½ m ω² A² cos²(ωt+φ); Total E = ½ k A² = ½ m ω² A². Energy oscillates between KE and PE; total constant.
-- NCERT, p. 7The trap: aspirants know that total energy in SHM is E = ½kA². They then see a question where amplitude doubles and confidently answer "energy doubles." It quadruples. Energy scales as the square of amplitude — and this is a high-frequency NEET distractor.
The concept. In simple harmonic motion, mechanical energy continuously converts between kinetic and potential forms. At the mean position (x = 0), all energy is kinetic: KE = ½mω²A². At the extreme positions (x = ±A), all energy is potential: PE = ½kA². At any intermediate displacement x:
The total is constant — independent of x, independent of time. This follows directly from the conservative nature of the restoring force (NCERT Class 11 Physics, Oscillations chapter, page 7).
Two critical facts from NCERT (Oscillations chapter, page 6): (1) KE and PE each oscillate at frequency 2ω (twice the oscillation frequency), and (2) their time-averaged values are equal, each ½E.
The amplitude-squared dependence is what catches students. Since E = ½kA², doubling A means E → 4E, not 2E. Tripling A means E → 9E. The period T = 2π√(m/k) does not depend on amplitude — but the energy emphatically does. This asymmetry is a common confusion (trap: period-amplitude independence does NOT mean energy-amplitude independence).
Watch-out for NEET: questions that change amplitude and ask for the new total energy, or ask at what displacement KE equals PE (answer: x = A/√2).
Select an option to see the explanation. Wrong answers show why your choice was tempting — and name the exact trap it exploits.
In simple harmonic motion, at which position is the kinetic energy maximum?
The total mechanical energy of a particle in ideal SHM (no damping) is:
In SHM, the kinetic energy and potential energy each oscillate with a frequency equal to:
A block on a frictionless surface oscillates on a spring with amplitude A and total energy E. If the amplitude is doubled to 2A (same spring, same mass), the new total energy is:
A particle in SHM has amplitude A. At what displacement from the mean position is the kinetic energy equal to the potential energy?
A spring-mass system has spring constant k = 200 N/m and oscillates with amplitude 0.10 m. The total energy of the system is:
A 0.50 kg block attached to a spring (k = 200 N/m) oscillates with amplitude 5.0 × 10⁻² m. What is the maximum speed of the block?
A particle executes SHM with amplitude A and angular frequency ω. At displacement x = A/2 from the mean position, the ratio of kinetic energy to potential energy is:
Pattern: Given a spring-mass system with changed amplitude, find the ratio of total energies. (Based on the amplitude-squared energy dependence — the core trap for this topic.)
Given
A spring-mass oscillator has mass m = 0.40 kg and spring constant k = 160 N/m. It oscillates first with amplitude A₁ = 0.050 m, then the amplitude is increased to A₂ = 0.15 m.
Required
Find the ratio E₂/E₁.
Concept
Total energy in SHM is E = ½kA². Energy depends on the square of amplitude. Spring constant and mass remain unchanged.
Formula
E = ½kA², so E₂/E₁ = A₂²/A₁².
Substitution
E₂/E₁ = (0.15)²/(0.050)² = 0.0225/0.0025
Calculation
E₂/E₁ = 9 Note: k and m are the same in both cases, so they cancel. The ratio depends purely on the amplitude ratio squared: (A₂/A₁)² = (0.15/0.050)² = 3² = 9.
Final answer
E₂/E₁ = 9. The new total energy is 9 times the original. Note on exact values: the ratio 3 (= 0.15/0.050) is exact arithmetic, and the squaring gives an exact integer 9. No sig-fig ambiguity arises.
Common trap
A student who thinks energy scales linearly with amplitude would answer E₂/E₁ = 3 (trap: period is amplitude-independent, but energy is NOT — it scales as A²). Another common error is confusing the energy ratio with the speed ratio (v_max ∝ Aω, so the speed ratio is 3, not 9).
Similar NEET-style question
A block oscillates on a spring with total energy 2.0 J and amplitude 4.0 × 10⁻² m. If the amplitude is halved to 2.0 × 10⁻² m (same spring), find the new total energy. [Answer: E_new = 2.0 × (1/2)² = 0.50 J] ---
KE(t) = ½ m ω² A² sin²(ωt+φ); PE(t) = ½ k x² = ½ m ω² A² cos²(ωt+φ); Total E = ½ k A² = ½ m ω² A². Energy oscillates between KE and PE; total constant.
-- NCERT, p. 7Velocity leads displacement by π/2: v = -A ω sin(ωt+φ). Acceleration leads displacement by π: a = -A ω² cos(ωt+φ) = -ω² x. KE max at x=0; PE max at x=±A.
-- NCERT, p. 6When 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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