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Mathematics LibreTexts

4.7: Resonance

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Resonance occurs when the frequency of the inhomogeneous term matches the frequency of the homogeneous solution. To illustrate resonance in its simplest embodiment, we consider the second-order linear inhomogeneous ode ..x+ω20x=fcosωt,x(0)=x0,.x(0)=u0.

Our main goal is to determine what happens to the solution in the limit ωω0.

The homogeneous equation has characteristic equation r2+ω20=0, so that r±=±iω0. Therefore, xh(t)=c1cosω0t+c2sinω0t.

To find a particular solution, we note the absence of a first-derivative term, and simply try x(t)=Acosωt.

Upon substitution into the ode, we obtain ω2A+ω20A=f, or A=fω20ω2.

Therefore, xp(t)=fω20ω2cosωt.

Our general solution is thus x(t)=c1cosω0t+c2sinω0t+fω20ω2cosωt, with derivative .x(t)=ω0(c2cosω0tc1sinω0t)fωω20ω2sinωt.

Initial conditions are satisfied when x0=c1+fω20ω2,u0=c2ω0, so that c1=x0fω20ω2,c2=u0ω0.

Therefore, the solution to the ode that satisfies the initial conditions is x(t)=(x0fω20ω2)cosω0t+u0ω0sinω0t+fω20ω2cosωt=x0cosω0t+u0ω0sinω0t+f(cosωtcosω0t)ω20ω2, where we have grouped together terms proportional to the forcing amplitude f.

Resonance occurs in the limit ωω0; that is, the frequency of the inhomogeneous term (the external force) matches the frequency of the homogeneous solution (the free oscillation). By L’Hospital’s rule, the limit of the term proportional to f is found by differentiating with respect to ω:

limωω0f(cosωtcosω0t)ω20ω2=limωω0ftsinωt2ω=ftsinω0t2ω0.

At resonance, the term proportional to the amplitude f of the inhomogeneous term increases linearly with t, resulting in larger-and-larger amplitudes of oscillation for x(t). In general, if the inhomogeneous term in the differential equation is a solution of the corresponding homogeneous differential equation, then the correct ansatz for the particular solution is a constant times the inhomogeneous term times t.

To illustrate this same example further, we return to the original ode, now assumed to be exactly at resonance, ..x+ω20x=fcosω0t, and find a particular solution directly. The particular solution is the real part of the particular solution of ..z+ω20z=feiω0t.

If we try zp=Ceiω0t, we obtain 0=f, showing that the particular solution is not of this form. Because the inhomogeneous term is a solution of the homogeneous equation, we should take as our ansatz zp=Ateiω0t.

We have .zp=Aeiω0t(1+iω0t),..zp=Aeiω0t(2iω0ω20t); and upon substitution into the ode ..zp+ω20zp=Aeiω0t(2iω0ω20t)+ω20Ateiω0t=2iω0Aeiω0t=feiω0t.

Therefore, A=f2iω0, and xp=Re{ft2iω0eiω0t}=ftsinω0t2ω0, the same result as (4.7.13).

Example 4.7.1

Find a particular solution of ..x3.x4x=5et.

Solution

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If we naively try the ansatz x=Aet, and substitute this into the inhomogeneous differential equation, we obtain A+3A4A=5, or 0=5, which is clearly nonsense. Our ansatz therefore fails to find a solution. The cause of this failure is that the corresponding homogeneous equation has solution xh=c1e4t+c2et, so that the inhomogeneous term 5et is one of the solutions of the homogeneous equation. To find a particular solution, we should therefore take as our ansatz x=Atet, with first- and second-derivatives given by .x=Aet(1t),..x=Aet(2+t).

Substitution into the differential equation yields Aet(2+t)3Aet(1t)4Atet=5et.

The terms containing t cancel out of this equation, resulting in 5A=5, or A=1. Therefore, the particular solution is xp=tet.


This page titled 4.7: Resonance is shared under a CC BY 3.0 license and was authored, remixed, and/or curated by Jeffrey R. Chasnov via source content that was edited to the style and standards of the LibreTexts platform.

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