<?xml version="1.0" encoding="utf-8" standalone="no"?>
<!DOCTYPE document PUBLIC "-//CNX//DTD CNXML 0.5 plus MathML//EN" "http://cnx.rice.edu/cnxml/0.5/DTD/cnxml_mathml.dtd">
<document xmlns="http://cnx.rice.edu/cnxml" xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" id="m10993">
  <name>Discrete-Time Processing of CT Signals</name>
  <metadata>
  <md:version>2.1</md:version>
  <md:created>2003/01/09</md:created>
  <md:revised>2003/02/28</md:revised>
  <md:authorlist>
      <md:author id="nowak">
      <md:firstname>Rob</md:firstname>
      <md:othername>"The Kid"</md:othername>
      <md:surname>Nowak</md:surname>
      <md:email>nowak@rice.edu</md:email>
    </md:author>
  </md:authorlist>

  <md:maintainerlist>
    <md:maintainer id="mjhaag">
      <md:firstname>Michael</md:firstname>
      
      <md:surname>Haag</md:surname>
      <md:email>mjhaag@rice.edu</md:email>
    </md:maintainer>
    <md:maintainer id="nowak">
      <md:firstname>Rob</md:firstname>
      <md:othername>"The Kid"</md:othername>
      <md:surname>Nowak</md:surname>
      <md:email>nowak@rice.edu</md:email>
    </md:maintainer>
  </md:maintainerlist>
  
  <md:keywordlist>
    <md:keyword>A/D</md:keyword>
    <md:keyword>analog</md:keyword>
    <md:keyword>CTFT</md:keyword>
    <md:keyword>D/A</md:keyword>
    <md:keyword>digital</md:keyword>
    <md:keyword>DTFT</md:keyword>
    <md:keyword>Fourier Transform</md:keyword>
    <md:keyword>LTI Systems</md:keyword>
  </md:keywordlist>

  <md:abstract>The module will provide analysis and examples of how a continuous-time signal is converted to a digital signal and processed.</md:abstract>
</metadata>

  <content>
    <section id="sec1">
      <name>DT Processing of CT Signals</name>

      <figure id="fig1">
	<name>DSP System</name>
	<media type="image/png" src="sec9_fig1.png"/>
      </figure>      
      
      <section id="sub1_s1">
	<name>Analysis</name>
	<para id="p1_s1">
	  
	  <equation id="eq1">
	    <m:math>
	      <m:apply>
		<m:eq/>
		<m:apply>
		  <m:ci type="fn"><m:msub>
		      <m:mi>Y</m:mi>
		      <m:mi>c</m:mi>
		    </m:msub></m:ci>
		  <m:ci>Ω</m:ci>
		</m:apply>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:ci type="fn"><m:msub>
			<m:mi>H</m:mi>
			<m:mi>LP</m:mi>
		      </m:msub></m:ci>
		    <m:ci>Ω</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:ci type="fn">Y</m:ci>
		    <m:apply>
		      <m:times/>
		      <m:ci>Ω</m:ci>
		      <m:ci>T</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:math>
	  </equation>

	  where we know that 
	  <m:math>
	    <m:apply>
	      <m:eq/>
	      <m:apply>
		<m:ci type="fn">Y</m:ci>
		<m:ci>ω</m:ci>
	      </m:apply>
	      <m:apply>
		<m:times/>
		<m:apply>
		  <m:ci type="fn">X</m:ci>
		  <m:ci>ω</m:ci>
		</m:apply>
		<m:apply>
		  <m:ci type="fn">G</m:ci>
		  <m:ci>ω</m:ci>
		</m:apply>
	      </m:apply>
	    </m:apply>
	  </m:math>
	  and 
	  <m:math>
	    <m:apply>
	      <m:ci type="fn">G</m:ci>
	      <m:ci>ω</m:ci>
	    </m:apply>
	  </m:math> is the frequency response of the DT LTI system.
	  Also, remember that 

	  <m:math display="block">
	    <m:apply>
	      <m:equivalent/>
	      <m:ci>ω</m:ci>
	      <m:apply>
		<m:times/>
		<m:ci>Ω</m:ci>
		<m:ci>T</m:ci>
	      </m:apply>
	    </m:apply>
	  </m:math>

	  So, 	  
	  
	  <equation id="eq2">
	    <m:math>
	      <m:apply>
		<m:eq/>
		<m:apply>
		  <m:ci type="fn"><m:msub>
		      <m:mi>Y</m:mi>
		      <m:mi>c</m:mi>
		    </m:msub></m:ci>
		  <m:ci>Ω</m:ci>
		</m:apply>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:ci type="fn"><m:msub>
			<m:mi>H</m:mi>
			<m:mi>LP</m:mi>
		      </m:msub></m:ci>
		    <m:ci>Ω</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:ci type="fn">G</m:ci>
		    <m:apply>
		      <m:times/>
		      <m:ci>Ω</m:ci>
		      <m:ci>T</m:ci>
		    </m:apply>
		  </m:apply>
		  <m:apply>
		    <m:ci type="fn">X</m:ci>
		    <m:apply>
		      <m:times/>
		      <m:ci>Ω</m:ci>
		      <m:ci>T</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:math>
	  </equation>
	  
	  where 
	  <m:math>
	    <m:apply>
	      <m:ci type="fn"><m:msub>
		  <m:mi>Y</m:mi>
		  <m:mi>c</m:mi>
		</m:msub></m:ci>
	      <m:ci>Ω</m:ci>
	    </m:apply>
	  </m:math> and 
	  <m:math>
	    <m:apply>
	      <m:ci type="fn"><m:msub>
		  <m:mi>H</m:mi>
		  <m:mi>LP</m:mi>
		</m:msub></m:ci>
	      <m:ci>Ω</m:ci>
	    </m:apply>
	  </m:math> are CTFTs and 
	  <m:math>
	    <m:apply>
	      <m:ci type="fn">G</m:ci>
	      <m:apply>
		<m:times/>
		<m:ci>Ω</m:ci>
		<m:ci>T</m:ci>
	      </m:apply>
	    </m:apply>
	  </m:math> and 
	  <m:math>
	    <m:apply>
	      <m:ci type="fn">X</m:ci>
	      <m:apply>
		<m:times/>
		<m:ci>Ω</m:ci>
		<m:ci>T</m:ci>
	      </m:apply>
	    </m:apply>
	  </m:math> are DTFTs.
	  
	  
	  <note type="Recall">
	    
	    <m:math display="block">
	      <m:apply>
		<m:eq/>
		<m:apply>
		  <m:ci type="fn">X</m:ci>
		  <m:ci>ω</m:ci>
		</m:apply>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:divide/>
		    <m:apply>
		      <m:times/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		    </m:apply>
		    <m:ci>T</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:sum/>
		    <m:bvar>
		      <m:ci>k</m:ci>
		    </m:bvar>
		    <m:uplimit>
		      <m:infinity/>
		    </m:uplimit>
		    <m:lowlimit>
		      <m:apply>
			<m:minus/>
			<m:infinity/>
		      </m:apply>
		    </m:lowlimit>
		    <m:apply>
		      <m:ci type="fn"><m:msub>
			  <m:mi>X</m:mi>
			  <m:mi>c</m:mi>
			</m:msub></m:ci>
		      <m:apply>
			<m:divide/>
			<m:apply>
			  <m:minus/>
			  <m:ci>ω</m:ci>
			  <m:apply>
			    <m:times/>
			    <m:cn>2</m:cn>
			    <m:pi/>
			    <m:ci>k</m:ci>
			  </m:apply>
			</m:apply>
			<m:ci>T</m:ci>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:math>
	    
	    OR
	    
	    <m:math display="block">
	      <m:apply>
		<m:eq/>
		<m:apply>
		  <m:ci type="fn">X</m:ci>
		  <m:apply>
		    <m:times/>
		    <m:ci>Ω</m:ci>
		    <m:ci>T</m:ci>
		  </m:apply>
		</m:apply>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:divide/>
		    <m:apply>
		      <m:times/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		    </m:apply>
		    <m:ci>T</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:sum/>
		    <m:bvar>
		      <m:ci>k</m:ci>
		    </m:bvar>
		    <m:uplimit>
		      <m:infinity/>
		    </m:uplimit>
		    <m:lowlimit>
		      <m:apply>
			<m:minus/>
			<m:infinity/>
		      </m:apply>
		    </m:lowlimit>
		    <m:apply>
		      <m:ci type="fn">
			<m:msub>
			  <m:mi>X</m:mi>
			  <m:mi>c</m:mi>
			</m:msub>
		      </m:ci>
		      <m:apply>
			<m:minus/>
			<m:ci>Ω</m:ci>
			<m:apply>
			  <m:times/>
			  <m:ci>k</m:ci>
			  <m:ci><m:msub>
			      <m:mi>Ω</m:mi>
			      <m:mi>s</m:mi>
			    </m:msub></m:ci>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:math>
	  </note>

	  Therefore our final output signal, 
	  <m:math>
	    <m:apply>
	      <m:ci type="fn"><m:msub>
		  <m:mi>Y</m:mi>
		  <m:mi>c</m:mi>
		</m:msub></m:ci>
	      <m:ci>Ω</m:ci>
	    </m:apply>
	  </m:math>, will be:

	  <equation id="eq4">
	    <m:math>
	      <m:apply>
		<m:eq/>
		<m:apply>
		  <m:ci type="fn"><m:msub>
		      <m:mi>Y</m:mi>
		      <m:mi>c</m:mi>
		    </m:msub></m:ci>
		  <m:ci>Ω</m:ci>
		</m:apply>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:ci type="fn"><m:msub>
			<m:mi>H</m:mi>
			<m:mi>LP</m:mi>
		      </m:msub></m:ci>
		    <m:ci>Ω</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:ci type="fn">G</m:ci>
		    <m:apply>
		      <m:times/>
		      <m:ci>Ω</m:ci>
		      <m:ci>T</m:ci>
		    </m:apply>
		  </m:apply>		  
		  <m:apply>
		    <m:times/>
		    <m:apply>
		      <m:divide/>
		      <m:apply>
			<m:times/>
			<m:cn>2</m:cn>
			<m:pi/>
		      </m:apply>
		      <m:ci>T</m:ci>
		    </m:apply>
		    <m:apply>
		      <m:sum/>
		      <m:bvar>
			<m:ci>k</m:ci>
		      </m:bvar>
		      <m:uplimit>
			<m:infinity/>
		      </m:uplimit>
		      <m:lowlimit>
			<m:apply>
			  <m:minus/>
			  <m:infinity/>
			</m:apply>
		      </m:lowlimit>
		      <m:apply>
			<m:ci type="fn"><m:msub>
			    <m:mi>X</m:mi>
			    <m:mi>c</m:mi>
			  </m:msub></m:ci>
			<m:apply>
			  <m:minus/>
			  <m:ci>Ω</m:ci>
			  <m:apply>
			    <m:times/>
			    <m:ci>k</m:ci>
			    <m:ci><m:msub>
				<m:mi>Ω</m:mi>
				<m:mi>s</m:mi>
			      </m:msub></m:ci>
			  </m:apply>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:math>
	  </equation>  
	 
	  Now, if 
	  <m:math>
	    <m:apply>
	      <m:ci type="fn"><m:msub>
		  <m:mi>X</m:mi>
		  <m:mi>c</m:mi>
		</m:msub></m:ci>
	      <m:ci>Ω</m:ci>
	    </m:apply>
	  </m:math> is bandlimited to 
	  
	  <m:math>
	    <m:interval>
	      <m:apply>
		<m:minus/>
		<m:apply>
		  <m:divide/>
		  <m:ci><m:msub>
		      <m:mi>Ω</m:mi>
		      <m:mi>s</m:mi>
		    </m:msub></m:ci>
		  <m:cn>2</m:cn>
		</m:apply>
	      </m:apply>
	      <m:apply>
		<m:divide/>
		<m:ci><m:msub>
		    <m:mi>Ω</m:mi>
		    <m:mi>s</m:mi>
		  </m:msub></m:ci>
		<m:cn>2</m:cn>
	      </m:apply>
	    </m:interval>
	  </m:math>
	  and we use the usual lowpass reconstruction filter in the
	  D/A, <cnxn target="fig2" strength="9"/>:
	</para>   
	
	<figure id="fig2">
	  <media type="image/png" src="sec9_fig2.png"/>
	</figure> 
	
	<para id="p2_s1">
	  Then,

	  <equation id="eq5">
	    <m:math>
	      <m:apply>
		<m:eq/>
		<m:apply>
		  <m:ci type="fn"><m:msub>
		      <m:mi>Y</m:mi>
		      <m:mi>c</m:mi>
		    </m:msub></m:ci>
		  <m:ci>Ω</m:ci>
		</m:apply>
		<m:piecewise>
		  <m:piece>
		    <m:apply>
		      <m:times/>
		      <m:apply>
			<m:ci type="fn">G</m:ci>
			<m:apply>
			  <m:times/>
			  <m:ci>Ω</m:ci>
			  <m:ci>T</m:ci>
			</m:apply>
		      </m:apply>		
		      <m:apply>
			<m:ci type="fn"><m:msub>
			    <m:mi>X</m:mi>
			    <m:mi>c</m:mi>
			  </m:msub></m:ci>
			<m:ci>Ω</m:ci>		    
		      </m:apply>
		    </m:apply>		
		    <m:apply>
		      <m:lt/>
		      <m:apply>
			<m:abs/>
			<m:ci>Ω</m:ci>
		      </m:apply>
		      <m:apply>
			<m:divide/>
			<m:ci><m:msub>
			    <m:mi>Ω</m:mi>
			    <m:mi>s</m:mi>
			  </m:msub></m:ci>
			<m:cn>2</m:cn>
		      </m:apply>
		    </m:apply>
		  </m:piece>
		  <m:otherwise>
		    <m:cn>0</m:cn>
		  </m:otherwise>
		</m:piecewise>
	      </m:apply>
	    </m:math>
	  </equation>
	</para>
      </section>

      <section id="sub2_s1">
	<name>Summary</name>
	<para id="p1_s2s1">
	  For bandlimited signals sampled at or above the Nyquist
	  rate, we can relate the input and output of the DSP system
	  by:

	  <equation id="eq6">
	   <m:math>
	      <m:apply>
		<m:eq/>
		<m:apply>
		  <m:ci type="fn"><m:msub>
		      <m:mi>Y</m:mi>
		      <m:mi>c</m:mi>
		    </m:msub></m:ci>
		  <m:ci>Ω</m:ci>
		</m:apply>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:ci type="fn"><m:msub>
			<m:mi>G</m:mi>
			<m:mi>eff</m:mi>
		      </m:msub></m:ci>
		    <m:ci>Ω</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:ci type="fn"><m:msub>
			<m:mi>X</m:mi>
			<m:mi>c</m:mi>
		      </m:msub></m:ci>
		    <m:ci>Ω</m:ci>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:math>
	  </equation>

	  where 
	  <m:math display="block">
	    <m:apply>
	      <m:eq/>
	      <m:apply>
		<m:ci type="fn"><m:msub>
		    <m:mi>G</m:mi>
		    <m:mi>eff</m:mi>
		  </m:msub></m:ci>
		<m:ci>Ω</m:ci>
	      </m:apply>
	      <m:piecewise>
		<m:piece>
		  <m:apply>
		    <m:ci type="fn">G</m:ci>
		    <m:apply>
		      <m:times/>
		      <m:ci>Ω</m:ci>
		      <m:ci>T</m:ci>
		    </m:apply>
		  </m:apply>
		  <m:apply>
		    <m:lt/>
		    <m:apply>
		      <m:abs/>
		      <m:ci>Ω</m:ci>
		    </m:apply>
		    <m:apply>
		      <m:divide/>
		      <m:ci><m:msub>
			  <m:mi>Ω</m:mi>
			  <m:mi>s</m:mi>
			</m:msub></m:ci>
		      <m:cn>2</m:cn>
		    </m:apply>
		  </m:apply>
		</m:piece>
		<m:otherwise>
		  <m:cn>0</m:cn>
		</m:otherwise>
	      </m:piecewise>
	    </m:apply>
	  </m:math>
	</para>

	<figure id="fig3">
	  <media type="image/png" src="sec9_fig3.png"/>
	</figure> 

	<section id="subsec">
	  <name>Note</name>
	  <para id="p3_s2s1">
	    
	    <m:math>
	      <m:apply>
		<m:ci type="fn"><m:msub>
		    <m:mi>G</m:mi>
		    <m:mi>eff</m:mi>
		  </m:msub></m:ci>
		<m:ci>Ω</m:ci>
	      </m:apply>
	    </m:math> is LTI if and only if the following two
	    conditions are satisfied:

	    <list id="list1" type="enumerated">
	      <item>
		<m:math>
		  <m:apply>
		    <m:ci type="fn">G</m:ci>
		    <m:ci>ω</m:ci>
		  </m:apply>
		</m:math> is LTI (in DT).
	      </item>

	      <item>
		<m:math>
		  <m:apply>
		    <m:ci type="fn"><m:msub>
			<m:mi>X</m:mi>
			<m:mi>c</m:mi>
		      </m:msub></m:ci>
		    <m:ci>T</m:ci>
		  </m:apply>
		</m:math> is bandlimited and sampling rate equal to or
		greater than Nyquist.  For example, if we had a simple
		pulse described by 
		
		<m:math display="block">
		  <m:apply>
		    <m:eq/>
		    <m:apply>
		      <m:ci type="fn"><m:msub>
			  <m:mi>X</m:mi>
			  <m:mi>c</m:mi>
			</m:msub></m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		    <m:apply>
		      <m:minus/>
		      <m:apply>
			<m:ci type="fn">u</m:ci>
			<m:apply>
			  <m:minus/>
			  <m:ci>t</m:ci>
			  <m:ci><m:msub>
			      <m:mi>T</m:mi>
			      <m:mn>0</m:mn>
			    </m:msub></m:ci>
			</m:apply>
		      </m:apply>
		      <m:apply>
			<m:ci type="fn">u</m:ci>
			<m:apply>
			  <m:minus/>
			  <m:ci>t</m:ci>
			  <m:ci><m:msub>
			      <m:mi>T</m:mi>
			      <m:mn>1</m:mn>
			    </m:msub></m:ci>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:math>
		
		where 
		<m:math>
		  <m:apply>
		    <m:gt/>
		    <m:ci><m:msub>
			<m:mi>T</m:mi>
			<m:mn>1</m:mn>
		      </m:msub></m:ci>
		    <m:ci><m:msub>
			<m:mi>T</m:mi>
			<m:mn>0</m:mn>
		      </m:msub></m:ci>
		  </m:apply>
		</m:math>.  If the sampling period 
		
		<m:math>
		  <m:apply>
		    <m:gt/>
		    <m:ci>T</m:ci>
		    <m:apply>
		      <m:minus/>
		      <m:ci><m:msub>
			  <m:mi>T</m:mi>
			  <m:mn>1</m:mn>
			</m:msub></m:ci>
		      <m:ci><m:msub>
			  <m:mi>T</m:mi>
			  <m:mn>0</m:mn>
			</m:msub></m:ci>
		    </m:apply>
		  </m:apply>
		</m:math>, 
		then some samples might "miss" the pulse while others
		might not be "missed."  This is what we term
		<term>time-varying behavior</term>.
	      </item>
	    </list>
	  </para>
	</section>
      </section>
      
      <example id="eg1">
	
	<figure id="fig4">
	  <media type="image/png" src="sec9_fig4.png"/>
	</figure>
	
	<para id="p1_eg1">
	  If 
	  <m:math>
	    <m:apply>
	      <m:gt/>
	      <m:apply>
		<m:divide/>
		<m:apply>
		  <m:times/>
		  <m:cn>2</m:cn>
		  <m:pi/>
		</m:apply>
		<m:ci>T</m:ci>
	      </m:apply>
	      <m:apply>
		<m:times/>
		<m:cn>2</m:cn>
		<m:ci>B</m:ci>
	      </m:apply>		
	    </m:apply>
	  </m:math> and 
	  <m:math>
	    <m:apply>
	      <m:lt/>
	      <m:ci><m:msub>
		<m:mi>ω</m:mi>
		<m:mn>1</m:mn>
	      </m:msub></m:ci>
	      <m:apply>
		<m:times/>
		<m:ci>B</m:ci>
		<m:ci>T</m:ci>
	      </m:apply>
	    </m:apply>
	  </m:math>, determine and sketch 
	  
	  <m:math>
	    <m:apply>
	      <m:ci type="fn"><m:msub>
		  <m:mi>Y</m:mi>
		  <m:mi>c</m:mi>
		</m:msub></m:ci>
	      <m:ci>Ω</m:ci>
	    </m:apply>
	  </m:math> using <cnxn target="fig4" strength="9"/>.

	</para>
      </example>
    </section>

    <section id="sec2">
      <name>Application: 60Hz Noise Removal</name>
      
      <figure id="fig5">
	<media type="image/png" src="sec9_fig5.png"/>
      </figure> 
      
      <para id="p1_s2">
	Unfortunately, in real-world situations electrodes also pick
	up ambient 60 Hz signals from lights, computers,
	<foreign>etc.</foreign>. In fact, usually this "60 Hz noise"
	is much greater in amplitude than the EKG signal shown in
	<cnxn target="fig5" strength="9"/>.  <cnxn target="fig6" strength="9"/> shows the EKG signal; it is barely noticeable
	as it has become overwhelmed by noise.
      </para>
      
      <figure id="fig6">
	<media type="image/png" src="sec9_fig6.png"/>
	<caption>
	  Our EKG signal, 
	  <m:math>
	    <m:apply>
	      <m:ci type="fn">y</m:ci>
	      <m:ci>t</m:ci>
	    </m:apply>
	  </m:math>, is overwhelmed by noise.
	</caption>	  
      </figure> 
      
      <section id="sub1_last">
	<name>DSP Solution</name>
	
	<figure id="fig7">
	  <media type="image/png" src="sec9_fig7.png"/>
	</figure> 

	<figure id="fig7b">
	  <media type="image/png" src="sec9_fig7b.png"/>
	</figure> 
	
      </section>

      <section id="sub2_last">
	<name>Sampling Period/Rate</name>
	<para id="p1_sl">
	  First we must note that 
	  <m:math>
	    <m:apply>
	      <m:abs/>
	      <m:apply>
		<m:ci type="fn">Y</m:ci>
		<m:ci>Ω</m:ci>
	      </m:apply>
	    </m:apply>
	  </m:math> is <term>bandlimited</term> to ±60 Hz.
	  Therefore, the minimum rate should be 120 Hz.  In order to
	  get the best results we should set 

	  <m:math display="block">
	    <m:apply>
	      <m:eq/>
	      <m:ci><m:msub>
		  <m:mi>f</m:mi>
		  <m:mi>s</m:mi>
		</m:msub></m:ci>
	      <m:apply>
		<m:times/>
		<m:ci>240</m:ci>
		<m:ci>Hz</m:ci>
	      </m:apply>
	    </m:apply>
	  </m:math>.

	  <m:math display="block">
	    <m:apply>
	      <m:eq/>
	      <m:ci><m:msub>
		  <m:mi>Ω</m:mi>
		  <m:mi>s</m:mi>
		</m:msub></m:ci>
	      <m:apply>
		<m:times/>
		<m:cn>2</m:cn>
		<m:pi/>
		<m:apply>
		  <m:times/>
		  <m:cn>240</m:cn>
		  <m:apply>
		    <m:divide/>
		    <m:ci>rad</m:ci>
		    <m:ci>s</m:ci>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:apply>
	  </m:math>

	</para>
	
	<figure id="fig8">
	  <media type="image/png" src="sec9_fig8.png"/>
	</figure> 
	
      </section>
      
      <section id="sub3_last">
	<name>Digital Filter</name>
	<para id="p1_sub3l">
	  Therefore, we want to design a digital filter that will
	  remove the 60Hz component and preserve the rest.
	</para>
	
	<figure id="fig9">
	  <media type="image/png" src="sec9_figL.png"/>
	</figure> 
	
      </section>

    </section>

  </content>  
</document>
