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*[[Computing_the_output_of_a_DT_system_using_the_Convolution_sum|A hub page listing ECE301 related pages discussing the DT convolution]]
 
*[[Computing_the_output_of_a_DT_system_using_the_Convolution_sum|A hub page listing ECE301 related pages discussing the DT convolution]]
 
*[[Media:ECE_301_Fall_2007_Ch2_pt1.pdf|Course notes for Chapter 2 (part 1) of Oppenheim Willsky (pdf)]] from [[ECE_301_(BoutinFall2007)|ECE301 Fall 2007]]
 
*[[Media:ECE_301_Fall_2007_Ch2_pt1.pdf|Course notes for Chapter 2 (part 1) of Oppenheim Willsky (pdf)]] from [[ECE_301_(BoutinFall2007)|ECE301 Fall 2007]]
*[[Media:ECE_301_Fall_2007_Ch2_pt2.pdf|Course notes for Chapter 2 (part 2) of Oppenheim Willsky (pdf)]] from [[ECE_301_(BoutinFall2007)|ECE301 Fall 2007]]
 
  
  

Revision as of 05:48, 2 February 2011

Lecture 8 Blog, ECE301 Spring 2011, Prof. Boutin

Friday January 28, 2011 (Week 3) - See Course Schedule.


In lecture 8, we showed that the output of a DT LTI system can be written as a convolution sum between the input signal and the unit impulse response of the system. This was done using a sequence of three observations. Similarly, we showed that the output of a DT LTI system can be written as a convolution integral between the input signal and the unit impulse response of the system. We covered one example of a DT convolution. An example of a CT convolution will be given in the next lecture.

Action items before the next lecture:

Relevant Rhea Pages


Previous: Lecture 7

Next: Lecture 9


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