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'''1.Impulse response'''<\n>
 
'''1.Impulse response'''<\n>
  
Joseph Fourier first represented  Fourier integral theorem in the following DOE:<\n>
+
Joseph Fourier first represented  Fourier integral theorem in the following DOE:
 +
<br>
  
 
[[Image:DOE1.jpg]][1]
 
[[Image:DOE1.jpg]][1]
Which is then introduced into the first delta function as following:<\n>
+
Which is then introduced into the first delta function as following:
 +
<br>
  
 
[[Image:DOE2.jpg]][1]
 
[[Image:DOE2.jpg]][1]
And the end end up with what mathematicians called Dirac delta function:<\n>
+
And the end end up with what mathematicians called Dirac delta function:
 +
<br>
  
 
[[Image:DOE3.jpg]] [1]
 
[[Image:DOE3.jpg]] [1]
 
[[Category:Fourier series]]
 
[[Category:Fourier series]]
 +
<br>
 
'''2.Fourier series'''
 
'''2.Fourier series'''
  
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[[Image:figrelena.jpg]]
 
[[Image:figrelena.jpg]]
 +
<br>
 
[[ECE301bonus2|Back to the 2nd bonus point opportunity, ECE301 Spring 2013]]
 
[[ECE301bonus2|Back to the 2nd bonus point opportunity, ECE301 Spring 2013]]

Revision as of 11:30, 11 March 2013

1.Impulse response<\n>

Joseph Fourier first represented Fourier integral theorem in the following DOE:

DOE1.jpg[1] Which is then introduced into the first delta function as following:

DOE2.jpg[1] And the end end up with what mathematicians called Dirac delta function:

DOE3.jpg [1]
2.Fourier series

The input x(t) is a function with a fundamental period x(t)= 1 from x= 0 to 1 and f(x)= -1 to 0, with a discontinuity at x=0. The following graphs from matlab represents Gibbs phenomena, as n increases the overshot decreases.

N=25.jpg N=50.jpg N=100.jpg
3.Filters

The upper is the Gaussian filter, while bottom is the unsharp.

Figrelena.jpg
Back to the 2nd bonus point opportunity, ECE301 Spring 2013

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

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