Fourier Analysis of Sawtooth Signal with To = 1

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SUMMARY

The forum discussion focuses on the Fourier analysis of a sawtooth signal with a period (To) of 1. The coefficients for the Fourier series are derived, specifically noting that for k=0, the coefficient a0 equals 1/2, and for k ≠ 0, the coefficient is given by a_k = j/(2πk). The discussion highlights the integration process required to compute these coefficients and emphasizes the importance of correctly applying integration by parts and evaluating boundary conditions. Participants also address common errors, such as sign mistakes and the need to recognize k as an integer in periodic functions.

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Homework Statement



Sawtooth signal with To = 1, at T=0, x = 0, at T=1, x =1

verify:
<br /> <br /> a_{k} = \left\{\begin{matrix}<br /> \frac{1}{2}, for k=0; &amp; \\\frac{j}{2\pi k}, for k \neq 0; <br /> &amp; <br /> \end{matrix}\right.<br /> <br />

Homework Equations



\frac{1}{T_{0}} \int_{0}^{T_{0}} te^{-j(2\pi/T_{0}))kt}dt

The Attempt at a Solution



for k = 0

a_{0} = \int_{0}^{1} t dt

a_{0} = \frac{1}{2} t^{2} from 0 to 1 = 1/2

for k != 0

\int_{0}^{1} te^{-j(2\pi) kt}dt

u = t
du = dt
dv = e^(-j2\pi kt)

v = \frac{-1}{j2\pi k}e^{-j2\pi kt}t * \frac{-1}{j2\pi k}e^{-j2\pi kt} - \int \frac{-1}{j2\pi k}e^{-j2\pi kt} dt

t * \frac{-1}{j2\pi k}e^{-j2\pi kt} - \frac{e^{-j2\pi kt}}{4\pi^2k^2}

-1/j = j

t * \frac{j}{2\pi k}e^{-j2\pi kt} - \frac{e^{-j2\pi kt}}{4\pi^2k^2}

e^{-j2\pi kt} (t \frac{j}{2\pi k} - \frac{1}{4\pi^2 k^2})

getting close but not seeing where to go from here.
 
Last edited:
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Check the integration by parts rules: You seem to have forgotten to evaluate the first part at the boundaries (in particular, if you integrate over t from 0 to 1, there is no way t should remain in the final expression)
\int_a^b u(x)v&#039;(x)\,dx = \left[u(x)v(x)\right]_a^b - \int_a^b u&#039;(x)v(x)\,dx,
first term on the right hand side.
 
Päällikkö said:
Check the integration by parts rules: You seem to have forgotten to evaluate the first part at the boundaries (in particular, if you integrate over t from 0 to 1, there is no way t should remain in the final expression)
\int_a^b u(x)v&#039;(x)\,dx = \left[u(x)v(x)\right]_a^b - \int_a^b u&#039;(x)v(x)\,dx,
first term on the right hand side.
\frac{je^{-j2\pi k} }{2\pi k} - \frac{e^{-j2\pi k} }{4\pi^2 k^2} - \frac{1}{4\pi^2 k^2}
 
You seem to have a sign error. Also, remember that k is an integer (a periodic function is mapped into a series in Fourier space), and you should be able to arrive at the result.
 
Okay, see the sign error but still not seeing how that is going to get
the other terms to fall out leaving just j/(2pik).
 
k is an integer. What is \exp(-j2\pi k) for k integer?
 
Thank you Paallikko, I did not have that one in my notes.
 

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