(One intermediate revision by one other user not shown)
Line 5: Line 5:
  
 
----
 
----
UNDER CONSTRUCTION
 
 
 
Having obtained the relationship between the DT Fourier transform of  <math>x_1[n]</math> and that of an upsampling of x[n] by a factor D in the previous lecture, we observed that, under certain circumstances, a low-pass filter could be applied to this upsampling so to obtain the signal  
 
Having obtained the relationship between the DT Fourier transform of  <math>x_1[n]</math> and that of an upsampling of x[n] by a factor D in the previous lecture, we observed that, under certain circumstances, a low-pass filter could be applied to this upsampling so to obtain the signal  
  
Line 26: Line 24:
 
[[2011_Fall_ECE_438_Boutin|Back to ECE438 Fall 2011]]
 
[[2011_Fall_ECE_438_Boutin|Back to ECE438 Fall 2011]]
  
[[Category:2011_Fall_ECE_438_Boutin]]
+
[[[Category:ECE438Fall2011Boutin]]  
[[Category:Blog]]
+
 
[[Category:ECE438]]
 
[[Category:ECE438]]
 +
[[Category:signal processing]]
 +
[[Category:ECE]]
 +
[[Category:Blog]]
 
[[Category:discrete Fourier transform]]
 
[[Category:discrete Fourier transform]]

Latest revision as of 06:24, 11 September 2013


Lecture 14 Blog, ECE438 Fall 2011, Prof. Boutin

Friday September 23, 2011 (Week 5) - See Course Outline.


Having obtained the relationship between the DT Fourier transform of $ x_1[n] $ and that of an upsampling of x[n] by a factor D in the previous lecture, we observed that, under certain circumstances, a low-pass filter could be applied to this upsampling so to obtain the signal

$ x_2[n]=x\left( n \frac{T_1}{D} \right) $.

We then began discussing the Discrete Fourier Transform (DFT).

Relevant Rhea pages

Action items



Previous: Lecture 13 Next: Lecture 15


Back to ECE438 Fall 2011

[[[Category:ECE438Fall2011Boutin]]

Alumni Liaison

Basic linear algebra uncovers and clarifies very important geometry and algebra.

Dr. Paul Garrett