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Damped Harmonic Oscillator Reference cheat sheet - grade 11-12

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A damped harmonic oscillator is a system that vibrates while losing mechanical energy to a resistive force such as friction or air resistance. This reference helps students connect the motion equation, exponential decay, frequency change, and energy loss in one organized place. It is useful for solving spring, pendulum, circuit analogy, and wave damping problems in upper high school physics.

The core model uses a restoring force proportional to displacement and a damping force proportional to velocity. For light damping, the object still oscillates, but its amplitude decreases like A(t)=A0eγtA(t) = A_0 e^{-\gamma t}. The most important ideas are the damping ratio, damped angular frequency, exponential energy decay, and whether the system is underdamped, critically damped, or overdamped.

Key Facts

  • The damped oscillator equation for linear damping is md2xdt2+bdxdt+kx=0m\frac{d^2x}{dt^2} + b\frac{dx}{dt} + kx = 0.
  • The natural angular frequency without damping is ω0=km\omega_0 = \sqrt{\frac{k}{m}}.
  • The damping constant used in many solutions is γ=b2m\gamma = \frac{b}{2m}.
  • For underdamped motion, the displacement is x(t)=A0eγtcos(ωdt+ϕ)x(t) = A_0 e^{-\gamma t}\cos(\omega_d t + \phi).
  • The damped angular frequency is ωd=ω02γ2\omega_d = \sqrt{\omega_0^2 - \gamma^2} for an underdamped oscillator.
  • The motion is underdamped when γ<ω0\gamma < \omega_0, critically damped when γ=ω0\gamma = \omega_0, and overdamped when γ>ω0\gamma > \omega_0.
  • The amplitude envelope decreases according to A(t)=A0eγtA(t) = A_0 e^{-\gamma t}.
  • The mechanical energy decreases approximately as E(t)=E0e2γtE(t) = E_0 e^{-2\gamma t} because energy is proportional to amplitude squared.

Vocabulary

Damping
Damping is the loss of mechanical energy from an oscillator due to resistive forces such as friction, drag, or internal resistance.
Damping force
A damping force is often modeled as Fd=bvF_d = -bv, where bb is the damping coefficient and the negative sign means the force opposes velocity.
Natural angular frequency
The natural angular frequency ω0=km\omega_0 = \sqrt{\frac{k}{m}} is the angular frequency the system would have with no damping.
Damped angular frequency
The damped angular frequency ωd=ω02γ2\omega_d = \sqrt{\omega_0^2 - \gamma^2} is the oscillation rate of an underdamped system.
Critical damping
Critical damping occurs when γ=ω0\gamma = \omega_0, giving the fastest return to equilibrium without oscillation.
Quality factor
The quality factor Q=ω02γQ = \frac{\omega_0}{2\gamma} measures how weakly damped an oscillator is, with larger QQ meaning slower energy loss.

Common Mistakes to Avoid

  • Using ω0\omega_0 instead of ωd\omega_d for the actual oscillation frequency is wrong because damping lowers the frequency in underdamped motion.
  • Forgetting that amplitude and energy decay at different rates is wrong because A(t)=A0eγtA(t) = A_0 e^{-\gamma t} but E(t)=E0e2γtE(t) = E_0 e^{-2\gamma t}.
  • Treating every damped system as oscillatory is wrong because overdamped and critically damped systems return to equilibrium without repeated oscillations.
  • Dropping the negative sign in Fd=bvF_d = -bv is wrong because the damping force must oppose the direction of motion.
  • Confusing the damping coefficient bb with the decay constant γ\gamma is wrong because they are related by γ=b2m\gamma = \frac{b}{2m}, not equal in general.

Practice Questions

  1. 1 A mass spring system has m=2.0kgm = 2.0\,\text{kg} and k=50N/mk = 50\,\text{N/m}. Find the natural angular frequency ω0\omega_0.
  2. 2 For a damped oscillator with m=1.5kgm = 1.5\,\text{kg} and b=0.60kg/sb = 0.60\,\text{kg/s}, calculate γ=b2m\gamma = \frac{b}{2m}.
  3. 3 An oscillator has ω0=10rad/s\omega_0 = 10\,\text{rad/s} and γ=3s1\gamma = 3\,\text{s}^{-1}. Find ωd\omega_d and classify the motion.
  4. 4 Explain why a critically damped car suspension is usually preferred over an underdamped or overdamped suspension.