Line 12: | Line 12: | ||
**[[Fourier_transform_cosine_CT_ECE301S11|Compute the Fourier transform of cos(2 pi t).]] | **[[Fourier_transform_cosine_CT_ECE301S11|Compute the Fourier transform of cos(2 pi t).]] | ||
**[[Fourier_transform_cosine_no2_CT_ECE301S11|Compute the Fourier transform of cos(2 pi t + pi/12).]] | **[[Fourier_transform_cosine_no2_CT_ECE301S11|Compute the Fourier transform of cos(2 pi t + pi/12).]] | ||
+ | **[[Fourier_transform_periodic_rectangular_pulse_train_CT_ECE301S11|Compute the Fourier transform of a rectangular pulse-train]] | ||
+ | **[[Fourier_transform_periodic_triangular_pulse_train_CT_ECE301S11|Compute the Fourier transform of a triangular pulse-train]] | ||
== Relevant Rhea Pages== | == Relevant Rhea Pages== |
Revision as of 11:07, 21 February 2011
Lecture 18 Blog, ECE301 Spring 2011, Prof. Boutin
Monday February 21, 2011 (Week 7) - See Course Schedule.
Today we obtained the formula for the Fourier transform of a periodic signal. We found that we cannot compute the Fourier transform of such signals using the integral formula. However, we were able to guess the answer and give a mathematical proof that our guess is correct.
We finished the lecture by discussing a few properties of the continuous-time Fourier transform.
Action items before the next lecture:
- Read Sections 4.4, 4.5, 4.7 in the book.
- Solve the following practice problem on CT Fourier transform.
Relevant Rhea Pages
Previous: Lecture 17
Next: Lecture 19