Harmonic Oscillation

Simple Harmonic Oscillation

When the only force applying on an object is proportional to its position F=kx the equation of motion is md2xdt2=kx The general solution is Bcos(ωt)+Csin(ωt) where ω=km

Damped Harmonic Oscillation

A damping force hinder an object's motion by exerting a force proportional to the object's velocity Fdamping=cdxdt the equation of motion is md2xdt2=kxcdxdt Let γ=c2m and ω20=km The equation of motion becomes d2xdt2+2γdxdt+ω20=0 Let x=eλt The equation of motion is (λ2+2γλ+ω20)eλt=0 To have a non-trivial solution, λ2+2γλ+ω20=0 Solve for λ λ=γ±γ2ω20 The general solution is x(t)=eγt[Bexp(γ2ω20t)+Cexp(γ2ω20t)]

Underdamping

When ω20>γ2 Let ωd=ω20γ2 The square root γ2ω20 is not real. The motion should be oscillation. The general solution is x(t)=eγt(Beiωdt+Ceiωdt)=Aeγtsin(ωdt+ϕ)

Critical damping

When ω20=γ2 So λ=γ Let x(t)=f(t)eγt. d2xdt2+2γdxdt+ω20=0d2fdt2+(2λ+2γ)dfdteλt+(λ2+2λγ+γ2)feλt=0d2fdt2=0f(t)=At+D The general solution is x(t)=(At+D)eγt

Overdamping

When ω20<γ2 The general solution is x(t)=Be(γq)t+Ce(γ+q)t where q=γ2ω20 The root is real so the motion is exponential rather than oscillation.

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