Physic Labs

Oscillations and waves

Introduction to simple harmonic motion

Study simple harmonic motion via the phase circle: verify x(t)=Acos⁡(ωt+φ)x(t) = A\cos(\omega t + \varphi), vmax⁡=Aωv_{\max} = A\omega, and a(t)=−ω2x(t)a(t) = -\omega^2 x(t) — acceleration always opposing and proportional to displacement.

High school

Equipment

  • 3D phase circle with a uniformly rotating point and its displacement projection
  • Sliders for amplitude A and frequency f
  • Initial-phase slider φ
  • Time plots of x, v, a and a Pause button

Procedure

  1. Read the phase circle and displacement plot

    Run the simulation: the red point rotates uniformly on the circle, and its projection on the axis is the displacement x=Acos⁡(ωt+φ)x = A\cos(\omega t + \varphi). Pause with the point at the top of the circle: the projection is at extreme, v=0v = 0, and aa is maximal with opposite sign.

  2. Vary A and f

    Raise amplitude A at fixed f: the x(t) curve grows taller, period unchanged. Raise f: the wave compresses, and vmax⁡=Aωv_{\max} = A\omega grows with both. Check the vmax⁡v_{\max} readout against AωA\omega with ω=2πf\omega = 2\pi f.

  3. Shift the initial phase

    Drag the φ slider: the whole x(t) trace slides in time while period and amplitude stay fixed — φ only sets the starting instant. Try φ = π/2: at t = 0 the body crosses equilibrium at maximum speed; predict the sign of v(0) before running.

Simulation

Experiment history

Simple harmonic motion emerged from Huygens's pendulum mechanics (Horologium Oscillatorium, 1673) and Brook Taylor's analysis of the vibrating string (1713), who proved the fundamental mode oscillates sinusoidally. Jean le Rond d'Alembert gave the wave equation (1747), and Joseph Fourier (1822) showed any periodic motion decomposes into sinusoids — the basis of the modern "mode" picture. Projecting uniform circular motion onto a diameter to produce harmonic motion is the classical geometric construction, tied to Fresnel's "reference circle" for adding light oscillations (1817). Today every system near stable equilibrium is approximated, to first order, by harmonic motion.

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