140 likes | 328 Views
Damped SHM. k. “Natural Frequency”. “Damping Parameter”. (rad/s). (s -1 ). m. “Damping Constant”. b. (kg/s). EOM: damped oscillator. Guess a complex solution:. “trivial solution”. Actually 2 equations:. Imaginary = 0. Real = 0. … also trivial !. Try a complex frequency:. Real.
E N D
Damped SHM k “Natural Frequency” “Damping Parameter” (rad/s) (s-1) m “Damping Constant” b (kg/s) EOM: damped oscillator
Guess a complex solution: “trivial solution” Actually 2 equations: Imaginary = 0 Real = 0 … also trivial !
Try a complex frequency: Real Imaginary A, f are free constants.
* amplitude decays due to damping * frequency reduced due to damping
How damped? Quality factor: unitless ratio of natural frequency to damping parameter Sometimes write solution in terms of wo and Q Sometimes write EOM in terms of wo and Q:
1. “Under Damped” or “Lightly Damped”: Oscillates at ~wo (slightly less) Looks like SHM (constant A) over a few cycles: wo= 1, g = .01, Q = 100, xo = 1 Amplitude drops by 1/e in Q/p cycles.
2. “Over Damped”: imaginary! part of A Still need two constants for the 2nd order EOM: No oscillations!
Over Damped wo= 1, g = 10, Q = .1, xo = 1
0 3 “Critically Damped”: …really just one constant, and we need two. Real solution:
Critically Damped wo= 1, g = 2, Q = .5, xo = 1 Fastest approach to zero with no overshoot.
Real oscillators lose energy due to damping. This can be represented by a damping force in the equation of motion, which leads to a decaying oscillation solution. The relative size of the resonant frequency and damping parameter define different behaviors: lightly damped, critically damped, or over damped. +