A body oscillating in Simple Harmonic Motion (SHM) follows the equation: x = A sin(ωt + φ) where x is displacement, A is amplitude, ω is angular frequency, t is time, and φ is initial phase.
Galileo discovered the isochronous nature of a pendulum in 1602 — that the time period is independent of amplitude (for small angles). This led to the invention of the pendulum clock by Huygens in 1656, revolutionising timekeeping.
Displacement: x = A sin(ωt + φ)
Or equivalently: x = A cos(ωt + φ)
Where:
By differentiating x = A sin(ωt + φ):
Velocity: v = dx/dt = Aω cos(ωt + φ)
Maximum velocity (at mean position): v_max = Aω
Acceleration: a = dv/dt = −Aω² sin(ωt + φ) = −ω²x
Maximum acceleration (at extreme position): a_max = Aω²
Key relationship: a = −ω²x (acceleration is proportional to displacement and opposite in direction — this IS the definition of SHM)
For a simple pendulum: T = 2π√(L/g) Where L = length, g = 9.8 m/s²
For a spring-mass system: T = 2π√(m/k) Where m = mass, k = spring constant
For any SHM: T = 2π/ω = 1/f
Kinetic Energy: KE = ½m(Aω)²cos²(ωt) = ½mω²(A²−x²) Potential Energy: PE = ½mω²x² Total Energy: E = KE + PE = ½mω²A² (constant!)
At mean position (x=0): KE is maximum, PE = 0 At extreme position (x=A): KE = 0, PE is maximum Total energy is conserved throughout SHM.
Velocity is maximum at the **mean position (x = 0)**. At this point, v_max = Aω. At the extreme positions (x = ±A), velocity = 0 because the body momentarily stops before reversing.
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