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Free vibration
no external force
Forced vibration
external force
Undamped vibration
no resistance
Damped vibration
resistance
General mechanical vibration model
my'' + cy' + ky = F(t), m - mass, c - damping, k - spring constant, F(t) - external force
I. Free Undamped Vibrations
my'' + ky = 0
Natural frequency and period
ω = √(k/m), T = 2π/ω
Free undamped solution
y = C₁sin(ωt) + C₂cos(ωt) = A sin(ωt + φ)
II. Forced Undamped Vibrations
y'' + ω²y = αcos(γt), ω - natural frequency, γ - applied frequency
No resonance
γ ≠ ω, z = α/(ω² − γ²) cos(γt)
Resonance
γ = ω, z = αt/(2ω) sin(ωt), unbounded oscillation
III. Damped Free Vibrations
y'' + αy' + βy = 0, α = c/m, β = k/m
Underdamped
α² − 4β < 0, y = e^(−αt/2)[C₁cos(ωt) + C₂sin(ωt)], oscillatory
Overdamped
α² − 4β > 0, y = C₁e^(r₁t) + C₂e^(r₂t), nonoscillatory
Critically damped
α² − 4β = 0, y = C₁e^(−αt/2) + C₂te^(−αt/2), nonoscillatory
IV. Forced Damped Vibrations
y'' + αy' + βy = acos(γt)
Transient and steady-state solutions
y = Yc + Z, Yc - transient/homogeneous and approaches 0, Z - steady-state/particular and remains