Energy in oscillators
Eₖ and Eₚ trade off as parabolas; their sum (E_T) stays constant.
For an (approximately) undamped oscillator, energy is continuously exchanged between kinetic and potential forms, but the total is conserved:
E_T = Eₖ + Eₚ = ½kA²
- At equilibrium (x=0): Eₖ is maximum, Eₚ = 0.
- At maximum displacement (x=±A): Eₖ = 0, Eₚ is maximum.
Combining these gives kinetic energy at any displacement:
Eₖ = E_T − Eₚ = ½k(A²−x²)
Types of damping
Light (blue), critical (red), heavy (green) damping compared.
- Light damping: each oscillation's amplitude is fractionally smaller than the last. Most real oscillators (springs, pendulums) are lightly damped.
- Critical damping: returns to equilibrium in the shortest possible time without overshooting — used where oscillation is undesirable (car suspension, compass needles).
- Heavy damping: returns to equilibrium slowly, without oscillating.
Finding the decay constant
Plotting lnA against t linearises the exponential decay.
Taking natural logs of A = A₀e^(−λt) gives a straight-line form:
ln A = ln A₀ − λt
Reading the graph: y-intercept = ln A₀; gradient = −λ. A steeper (more negative) gradient means a larger decay constant — faster damping.