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JEE · NEET Physics

Class 11 · Chapter 14

Oscillations

Overview, notes, short notes, formula sheet, daily practice problems, previous year questions, and videos for this chapter — all in one place.

Oscillations Formula Sheet

9 formulas across 3 topics in Oscillations.

1 min read

Updated 2026-07-04 · v1.0.0

SHM — Equation of Motion & Kinematics

SHM is defined by one property: restoring acceleration proportional to displacement, a = −ω²x. Spot that, and T = 2π/ω follows instantly.

a = −ω²x; x = A sin(ωt + φ); T = 2π/ω

Defining equation and solution of SHM

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
ωangular frequencyrad/s[T⁻¹]
Aamplitudem[L]
φinitial phaserad[M⁰L⁰T⁰]
Ttime periods[T]

Valid when

  • a ∝ −x is the TEST for SHM — check it before quoting any period formula

Common mistakes

  • Time from mean to extreme is T/4, but mean to A/2 takes only T/12 — SHM is fast near the mean, slow near the extremes

v = ω√(A² − x²); a = −ω²x

Velocity and acceleration at displacement x

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Differentiating x(t), then eliminating t

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
vspeed at displacement xm/s[LT⁻¹]
xdisplacement from the mean positionm[L]

Valid when

  • v(max) = ωA at the mean position; a(max) = ω²A at the extremes
  • v and a are 90° out of phase; a and x are 180° out of phase

Common mistakes

  • At the extreme, v = 0 but a is MAXIMUM — zero speed never means zero acceleration in SHM

Worth remembering

  • SHM is the projection of uniform circular motion on a diameter — the reference-circle picture solves every phase/timing question

Oscillating Systems — Springs & Pendulums

Every system reduces to finding its ω. Spring: √(k/m). Pendulum: √(g/L). Everything else is variations on these two.

T = 2π √(m/k)

Period of a spring-mass system

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F = −kx compared with F = −mω²x

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
moscillating masskg[M]
kspring constantN/m[MT⁻²]

Valid when

  • Independent of gravity — the same on Earth, in a lift, or in orbit
  • Vertical spring: gravity only SHIFTS the mean position, period unchanged

Common mistakes

  • Cutting a spring into n equal parts makes each piece n times STIFFER (k' = nk), so the period drops by √n

Series: 1/k(eq) = 1/k₁ + 1/k₂; Parallel: k(eq) = k₁ + k₂

Combination of springs

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
k(eq)equivalent spring constantN/m[MT⁻²]

Valid when

  • OPPOSITE of resistors: springs side-by-side (or one on each side of the mass) ADD; end-to-end combine reciprocally

Common mistakes

  • A mass between two springs attached to opposite walls is a PARALLEL combination — both springs push it back together

T = 2π √(L/g)

Period of a simple pendulum

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Restoring torque −mgL sinθ ≈ −mgLθ for small angles

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Llength from pivot to the bob's centrem[L]
geffective gravitational accelerationm/s²[LT⁻²]

Valid when

  • Small angles only (sinθ ≈ θ)
  • Independent of the bob's mass
  • In an accelerating frame use g(eff): lift up → g + a; free fall → T infinite (no oscillation)

Common mistakes

  • The seconds pendulum has T = 2 s (not 1 s) — one second per HALF swing, L ≈ 1 m on Earth

T = 2π √(I/(mgd))

Period of a physical (compound) pendulum

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Imoment of inertia about the pivotkg·m²[ML²]
ddistance from pivot to the centre of massm[L]

Valid when

  • Reduces to the simple pendulum when I = mL² and d = L
  • Rod pivoted at one end: T = 2π√(2L/3g)

Worth remembering

  • A floating cylinder pushed down, liquid in a U-tube, and a ball in a spherical bowl all execute SHM — derive ω from a = −ω²x each time rather than memorising

NEET repeats pendulum-in-lift and spring-cutting; JEE Advanced favours energy-method derivations of ω for unusual systems.

Energy in SHM, Damping & Resonance

Total energy in SHM is constant and proportional to A² — kinetic and potential merely trade places twice every period.

E = ½kA² = ½mω²A²; KE = ½mω²(A² − x²); PE = ½mω²x²

Energy in SHM

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KE + PE at any x, using v = ω√(A² − x²)

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Etotal mechanical energyJ[ML²T⁻²]
Aamplitudem[L]

Valid when

  • KE = PE at x = A/√2, not at A/2
  • KE and PE each oscillate at TWICE the SHM frequency

Common mistakes

  • Doubling the amplitude quadruples the energy — E ∝ A²

x = A e^(−bt/2m) cos(ω't + φ)

Damped oscillation

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
bdamping constant (F(damp) = −bv)kg/s[MT⁻¹]
ω'damped angular frequency √(k/m − b²/4m²)rad/s[T⁻¹]

Valid when

  • Amplitude decays exponentially; energy decays as e^(−bt/m) — twice as fast as amplitude

Resonance: driving frequency = natural frequency (ω(d) = ω₀)

Forced oscillations and resonance

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
ω(d)driving (forcing) frequencyrad/s[T⁻¹]
ω₀natural frequency of the systemrad/s[T⁻¹]

Valid when

  • Steady state: the system oscillates at the DRIVING frequency, not its own
  • Amplitude peaks at resonance; lighter damping → sharper, taller peak

Worth remembering

  • Soldiers break step on bridges to avoid resonance — the Tacoma Narrows collapse is the textbook cautionary tale

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