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The equation of motion for a spring-mass system excited by a harmonic force is

\[ M\ddot{x} + Kx = F\cos(\omega t), \]

where \(M\) is the mass, \(K\) is the spring stiffness, \(F\) is the force amplitude and \(\omega\) is the angular frequency of excitation. Resonance occurs when \(\omega\) is equal to

  • A.\(\sqrt{\frac{M}{K}}\)
  • B.\(\frac{1}{2\pi}\sqrt{\frac{K}{M}}\)
  • C.\(2\pi\sqrt{\frac{K}{M}}\)
  • D.\(\sqrt{\frac{K}{M}}\)

Answer: D

Resonance occurs at \(\omega = \sqrt{K/M}\).

Resonance is excitation at the natural frequency of the undamped system. The free equation \(M\ddot{x} + Kx = 0\) gives \(\omega_{n} = \sqrt{K/M}\) in rad/s, and the forced amplitude \(F/(K - M\omega^{2})\) grows without limit as \(\omega\) approaches it.

\(\frac{1}{2\pi}\sqrt{K/M}\) is the same natural frequency in hertz, but \(\omega\) is an angular frequency, so the units do not match. \(2\pi\sqrt{K/M}\) multiplies where it should not, and \(\sqrt{M/K}\) is inverted (it has units of time).

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