Coefficients of Fourier series for periodically driven oscillators

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SUMMARY

The discussion focuses on calculating the Fourier coefficients for a periodically driven oscillator subjected to a triangular periodic force with a period of τ = 2. The parameters include a natural period τ₀ = 2, a damping parameter β = 0.1, and a maximum drive strength fmax = 1. The Fourier coefficients are derived using the integral formula fn = (2/τ)∫-τ/2τ/2 f(t)cos(nωt)dt, where ω = 2π/τ. The final expression for the coefficients is fn = 4/((nπ)²), which is crucial for plotting the long-term motion x(t).

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Oijl
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Homework Statement


An oscillator is driven by a triangular periodic force (if that makes sense), which has period \tau = 2.

(a) Find the long-term motion x(t), assuming the following parameters: natural period \tau[naught] = 2 (that is, \omega[naught] = π), damping parameter ß = 0.1, and maximum drive strength fmax = 1. Find the coefficients in the Fourier series for x(t) and plot the sum of the first four terms in the series for 0 <= t <= 6.

Homework Equations





The Attempt at a Solution



For starters: the Fourier coefficients, An (A sub n), I see in my book the equation for. It has in it f sub n, omega naught, omega, beta, and n. n is easy, beta is given, omega naught is given, but omega and f sub n confuse me. I would have thought, that since omega = (2*pi)/(tau), that, with a period of 2, omega would equal pi. But that doesn't seem correct, and, also, I don't know how to find f sub n.

Further: if anyone knows the program Matlab well enough, could you share how I would be able to graph this? I only first began my relationship with the program last night (early this morning, really).

If what I'm asking doesn't make sense, sorry. Chalk it up to my sleeplessness.
 
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I think the fn's are the Fourier coefficients for the driving force.
 
Yes, the driving force f(t), which is f(t) = sum{fn*cos(wnt)}

But I'm really bad at this stuff and I don't know how to know the fn's.
 
OK, you're only using cosine terms, so the triangle wave must be symmetric about t=0. (If it's not, you'll need to use both the sine and cosine terms.)

You need to calculate

f_n = \frac{2}{\tau}\int_{-\tau/2}^{\tau/2} f(t)\cos(n\omega t)dt

where \omega=2\pi/\tau. If you're having problems doing this integral, post what you have so far or a more specific question so we can see where you're getting stuck.
 
Hmmm... so f(t) over that interval will be fmax, ehe? So:

fn = ((8*fmax*n*pi)/(tau^2))sin((2*n*pi*∆tau)/(tau))
So that in this case, where
tau = 2
fmax = 1
∆tau =? 1,
fn = (2*pi*n)sin(pi*n), so
fn = 0 for any n because of the sin function.

But they're not all zero.
 
Oijl said:
Hmmm... so f(t) over that interval will be fmax, ehe?
No, that would be a constant function, not a triangle wave. You first need to find a function of t that describe the triangle wave.
 
Is that so? But that would be, like,
f(t) = t
for 2n+1 <= t < 2n+2, where n is an integer, and
f(t) = -t
for 2n <= t < 2n+1

So should I just work it out differently for different n's?
 
You'll have to define it in a piecewise way, but you only have to define it from t=-\tau/2 to t=+\tau/2, because that's the interval over which you are integrating.

I suggest you sketch it so you get the correct equations for the two pieces.
 
I don't get it. The answer is that

fn = 4/((n*pi)^2),

but I can't get to that point from this.
 
  • #10
What do you have for f(t)?
 

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