(16 intermediate revisions by 4 users not shown)
Line 1: Line 1:
[[Category:ECE438Spring2009mboutin]][[Category:ECE438Spring2009mboutin:CourseNotes:Lecture1]]
+
[[Category:ECE]]
 +
[[Category:ECE438]]
 +
[[Category:signal processing]]
 +
[[Category:ECE438Spring2009mboutin]]
 +
[[Category:lecture notes]]
  
== ECE438 Course Notes January 14, 2009 ==
+
=Lecture Notes for [[ECE438]] Spring 2009, [[user:mboutin|Prof. Boutin]]=
 
+
*[[CourseNotes1_(BoutinSpring2009)|Course Notes Lecture 1 Jan. 14, 2009]]
1)Definitions
+
*[[CourseNotes2_(BoutinSpring2009)|Course Notes Lecture 2 Jan. 16, 2009]]
 
+
*[[CourseNotes3_(BoutinSpring2009)|Course Notes Lecture 3 Jan. 21, 2009]]
ECE438 is about digital signals and systems
+
*[[CourseNotes4_(BoutinSpring2009)|Course Notes Lecture 4 Jan. 23, 2009]]
 
+
*[[CourseNotes6_(BoutinSpring2009)|Course Notes Lecture 6 Jan. 28, 2009]]
2) Digital Signal = a signal that can be represented by a sequence of 0's and 1's.
+
*[[CourseNotes16_(BoutinSpring2009)|Course Notes Lecture 16 Feb. 23, 2009]]
so the signal must be DT X(t) = t, i.e. need x(n), n belongs to Z
+
*[[CourseNotes20_(BoutinSpring2009)|Course Notes Lecture 20 Mar. 11, 2009]]
 
+
*[[CourseNotes30_(BoutinSpring2009)|Course Notes Lecture 30 Apr. 17, 2009]]
Signal values must be discrete
+
----
 
+
[[ECE438_(BoutinFall2009)|Back to ECE438, Spring 2009]]
-<math>x(n) \in {0,1}</math> <-- binary valued signal
+
<br/><math>x(n) \in {0,1,2,...,255}</math> <-- gray scale valued signal
+
 
+
 
+
Another example of digital signal
+
 
+
-the pixels in a bitmap image (grayscale) can have a value of 0,1,2,...,255 for each individual pixel.
+
--If you concatenate all the rows of the image you can convert it to a 1 dimensional signal.
+
i.e. <math>x = (row1,row2,row3)</math>
+
 
+
2D Digital signal = signal that can be represented by an array of 0's and 1's
+
 
+
<u>example</u>: 128x128 gray scale image<br/>
+
<math>p_{ij} \in {0,...,255}</math>
+
 
+
matrix <math>A_{ij} = p_{ij}</math> of size 128x128 <br/>
+
 
+
[[Image:Vip_logo.jpg| 70px| left]]
+
Digital signals play an important roll in forensics applications such as: watermarking, image identification, and forgery detection among many others. Go to [http://cobweb.ecn.purdue.edu/~prints/publications.shtml PSAPF] and [http://cobweb.ecn.purdue.edu/~vip/teams/sensor_forensics.html VIP's Sensor Forensics] to find out more information about these applications.
+
 
+
<strong>Digital Systems</strong> = system that can process a ditital signal.<br/>
+
E.g.
+
<ul>
+
<li>Software (MATLAB,C, ...) </li>
+
<li>Firmware</li>
+
<li>Digital Hardware</li>
+
</ul>
+
 
+
== Advantages of Digital Systems ==
+
<ul>
+
<li>precise,reproducable</li>
+
<li>easier to store data</li>
+
<li>easier to build:
+
  <ul>
+
    <li>just need to represent 2 states instead of a continuous range of values</li>
+
  </ul>
+
</li>
+
</ul>
+
 
+
<strong>Software based digital systems</strong>
+
<ul>
+
<li>easier to build</li>
+
<li>cheap to build</li>
+
<li>adaptable</li>
+
<li>easy to fix/upgrade</li>
+
</ul>
+
 
+
<strong>Hardware-based digital systems</strong>
+
<ul>
+
<li>fast.</li>
+
 
+
</ul>
+
<table border="1px">
+
<tr>
+
<td  width="50%" align="center" valign="top">
+
<strong>Continuous time world</strong>
+
<ul>
+
<li>most natural signals live here</li>
+
<li>things are easy to write, understand, conceptualize</li>
+
 
+
</ul>
+
</td>
+
<td width="50%" align="center" valign="top">
+
<strong>Digital World</strong>
+
<ul>
+
<li>digital media signals live here along with computers, MATLAB, digital circuits</li>
+
</ul>
+
</td>
+
</tr>
+
</table>
+
<p>These world are brought together using sampling & quantization, as well as reconstruction</p>
+
 
+
== Signal Characteristics ==
+
<ul>
+
  <li>Deterministic vs. random
+
    <ul>
+
      <li>x(t) well defined , s.a. <math>x(t) =  e^{j\pi t}</math></li>
+
      <li>x(n) well defined , s.a. <math>x(n) = j^{n}</math> <br/>ex: Lena's image</li>
+
    </ul>
+
  </li>
+
  <li>Random
+
    <ul>
+
      <li>x(t) drawn according to some distribution</li>
+
      <li>example: x(t) white noise<br/>x = rand(10) (almost) random</li>
+
    </ul>
+
  </li>
+
</ul>
+
 
+
<ul>
+
  <li>Periodic vs. non-periodic
+
  <ul><li> if <math>\exists</math> positive T such that x(t+T) = x(t),<math>\forall t</math> then we say that x(t) is periodic with period T</li></ul>
+
  </li>
+
</ul>
+
 
+
== ECE438 Course Notes January 16, 2009 ==
+
 
+
<p><strong>Todays Goals</strong>
+
  <ul>
+
    <li>Signal Characteristics</li>
+
    <li>Signal Transformations</li>
+
    <li>Special Signals</li>
+
    <li>Singularity Functions</li>
+
  </ul>
+
</p>
+
 
+
<p><strong>right sided signal: </strong><br/>
+
<math>\exists t_{min} (n_{min})</math> such that <math>x(t) = 0</math> when <math>t < t_{min}</math>
+
</p>
+
 
+
<p><strong>left sided signal: </strong><br/>
+
<math>\exists t_{max} (n_{max})</math> such that <math>x(t) = 0</math> when <math>t > t_{max}</math><br/>
+
if <math>t_{max} \leq 0</math> we say the signal is <u>anticausal</u>
+
</p>
+
 
+
<p><strong>two sided (mixed causal):</strong><br/>
+
neither left sided nor right sided
+
</p>
+
 
+
<p><strong>Finite Duration Signal: </strong><br/>
+
both right and left sided, <math>\exists t_{min},t_{max}</math> such that <math>x(t) = 0</math> for <math>t > t_{max}</math> and <math>t < t_{min}</math>
+
</p>
+
 
+
<h3>Signal Metrics</h3>
+
<br/>
+
<ul style="list-style:none;">
+
  <li><strong>Signal Energy</strong>
+
    <ul style="list-style:none;">
+
      <li>
+
        <p><math>E_x = \int_{-\infty}^{\infty} |x(t)|^2\,dt</math> for ct (continuous time)</p>
+
        <p><math>E_x = \sum_{n=-\infty}^{\infty} |x(n)|^2</math> for dt (discrete time)</p>
+
      </li>
+
    </ul>
+
  </li>
+
  <li><strong>Signal Power</strong>
+
    <ul style="list-style:none;">
+
      <li>
+
        <p><math>P_x = \lim_{T \Rightarrow \infty}\frac{1}{2T}\int_{-T}^{T} |x(t)|^2\,dt</math> for ct (continuous time)</p>
+
        <p><math>P_x = \lim_{N \Rightarrow \infty}\sum_{n=-N}^{N} |x(n)|^2</math> for ct (continuous time)</p>
+
        <p>note: for periodic signals <br/>
+
        <math>P_x = \frac{1}{N}\sum_{n=0}^{N-1}|x(n)|^2</math>
+
        </p>
+
      </li>
+
    </ul>
+
  </li>
+
  <li><strong>Signal RMS (root-mean-square)</strong>
+
    <ul style="list-style:none;">
+
      <li>
+
      <math>X_{rms} = \sqrt{P_x}</math>
+
      </li>
+
    </ul>
+
  </li>
+
  <li><strong>Signal Magnitude</strong>
+
    <ul style="list-style:none;">
+
      <li>
+
        <p><math>m_x = max|x(t)|</math>, for CT</p>
+
        <p><math>m_x = max|x(n)|</math>, for DT</p>
+
        <p> if <math>m_x < \infty</math>, we say signal is bounded</p>
+
      </li>
+
    </ul>
+
  </li>
+
  <li><strong>Scaling (<math>y(t) = x(\frac{t}{a})</math>)</strong>
+
    <ul style="list-style:none;">
+
      <li>
+
        <p>note: y(0) = x(0), fixed point at t=0<br/>
+
        if a > 1, graph will narrow<br/>
+
        if a < 1, graph will expand<br/><br/>
+
        <font style="color:red;">if a>1 will not work for digital signals</font>
+
        </p><br/>
+
        <p><strong>Down Sampler:</strong><br/>
+
          <math>y(n) = x(Dn)</math>, D = integer > 1<br/>
+
          <math>x(n) \Rightarrow D\Downarrow \Rightarrow y(n)</math>
+
        </p>
+
        <p><strong>Up Sampler:</strong> <math>x(n) \Rightarrow D\Uparrow \Rightarrow y(n)</math><br/>
+
          <math>y(n) = x(\frac{n}{D})</math>, if n/D is an integer
+
        </p>
+
        <p><strong>Scaling and Shifting</strong> <math>y(t) = x(\frac{t}{a}-t_0)</math><br/>
+
          note: <math>y(0) = x(-t_0)</math>
+
        </p>
+
      </li>
+
    </ul>
+
  </li>
+
</ul>
+

Latest revision as of 06:37, 16 September 2013


Lecture Notes for ECE438 Spring 2009, Prof. Boutin


Back to ECE438, Spring 2009

Alumni Liaison

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

Dr. Paul Garrett