Physics · lesson 2 of 4
Driven oscillations, damping and resonance
A linear mass-spring oscillator obeys mx″+kx=0. Its natural angular frequency is sqrt(k/m), not k/m.
Learn the ideas
Prerequisites: Second-order differential equations and complex numbers.
Free motion
A linear mass-spring oscillator obeys mx″+kx=0. Its natural angular frequency is sqrt(k/m), not k/m.
Damping
A viscous damping force −bx′ converts the equation to mx″+bx′+kx=0. In underdamping, the oscillation envelope decays exponentially.
Driving
A periodic external force can transfer energy to the oscillator. The steady response depends on drive frequency, damping and phase.
Resonance
A finite drive does not imply infinite amplitude in a damped physical oscillator. Transient motion and nonlinear limits matter.
Worked examples
For m=2 kg and k=18 N/m, find the undamped angular frequency.
ω0=sqrt(k/m)=sqrt(9).
3 rad/s
Which force represents linear viscous damping?
The force opposes velocity and removes mechanical energy.
−b times velocity with b positive
Check your understanding
8 questionsDecimals or fractions are accepted for numeric answers. Proofs and written responses use sample answers and require human marking. This is practice, not a protected examination.
Further reading and review references
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