Mechanical Vibrations

Mechanical Vibrations

Vibration is the periodic motion of a body or system of connected bodies displaced from a position of equilibrium.

Free Undamped Vibrations

Consider a block of mass mm attached to a spring of stiffness kk.

Equation of Motion

mx¨+kx=0m \ddot{x} + k x = 0 The solution is simple harmonic motion: x(t)=Asin(ωnt)+Bcos(ωnt)x(t) = A \sin(\omega_n t) + B \cos(\omega_n t)

Key Parameters

  • Natural Circular Frequency: ωn=km\omega_n = \sqrt{\frac{k}{m}} (rad/s)
  • Natural Frequency: fn=ωn2πf_n = \frac{\omega_n}{2\pi} (Hz)
  • Period: τ=1fn=2πωn=2πmk\tau = \frac{1}{f_n} = \frac{2\pi}{\omega_n} = 2\pi \sqrt{\frac{m}{k}} (s)

Simple Pendulum

For small angles (sinθθ\sin \theta \approx \theta):

  • ωn=gL\omega_n = \sqrt{\frac{g}{L}}
  • Period τ=2πLg\tau = 2\pi \sqrt{\frac{L}{g}}

Damped Free Vibrations

If a viscous damper (cc) is added: mx¨+cx˙+kx=0m \ddot{x} + c \dot{x} + k x = 0

  • Critical Damping Coefficient (ccc_c): cc=2mωnc_c = 2m\omega_n
  • Damping Ratio (ζ\zeta): ζ=c/cc\zeta = c / c_c

If ζ<1\zeta < 1 (underdamped), the system oscillates with decreasing amplitude.

Example: Spring-Mass Period

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