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=−kx−cdxdt
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±√γ2−ω20
The general solution is
x(t)=eγt[Bexp(√γ2−ω20t)+Cexp(−√γ2−ω20t)]
Underdamping
When
ω20>γ2
Let
ωd=√ω20−γ2
The square root
√γ2−ω20 is not real. The motion should be oscillation. The general solution is
x(t)=e−γt(Beiωdt+Ce−iωdt)=Ae−γtsin(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)e−γt
Overdamping
When
ω20<γ2
The general solution is
x(t)=Be−(γ−q)t+Ce−(γ+q)t
where
q=√γ2−ω20
The root is real so the motion is exponential rather than oscillation.
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