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<!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:m="http://www.w3.org/1998/Math/MathML" xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:bib="http://bibtexml.sf.net/" id="m0085">
  <name>Amplitude Modulation</name>

  <metadata>
  <md:version>2.5</md:version>
  <md:created>2000/08/14</md:created>
  <md:revised>2004/08/04 15:20:22.538 GMT-5</md:revised>
  <md:authorlist>
      <md:author id="dhj">
      <md:firstname>Don</md:firstname>
      
      <md:surname>Johnson</md:surname>
      <md:email>dhj@rice.edu</md:email>
    </md:author>
  </md:authorlist>

  <md:maintainerlist>
    <md:maintainer id="dhj">
      <md:firstname>Don</md:firstname>
      
      <md:surname>Johnson</md:surname>
      <md:email>dhj@rice.edu</md:email>
    </md:maintainer>
    <md:maintainer id="montgom">
      <md:firstname>Joe</md:firstname>
      
      <md:surname>Montgomery</md:surname>
      <md:email>montgom@rice.edu</md:email>
    </md:maintainer>
  </md:maintainerlist>
  
  

  <md:abstract>Understanding and performing amplitude modulation through Fourier methods.</md:abstract>
</metadata>

  <content>

    <example id="ampmod">
      <para id="AmplitudeModulation"> 
	In communications, a very important operation on a signal  
	<m:math>
	  <m:apply>
	    <m:ci type="fn">s</m:ci>
	    <m:ci>t</m:ci>
	  </m:apply>
	</m:math>
	is to <term>amplitude modulate </term>it.  Using this operation
	more as an example rather than elaborating the communications
	aspects here, we want to compute the Fourier
	transform—the spectrum—of
	<equation id="eq1">
	  <m:math>
	    <m:apply>
	      <m:times/>
	      <m:apply>
		<m:plus/>
		<m:cn>1</m:cn>
		<m:apply>
		  <m:ci type="fn">s</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:apply>
	      <m:apply>
		<m:cos/>	    
		<m:apply>
		  <m:times/>
		  <m:cn>2</m:cn>
		  <m:pi/>
		  <m:ci><m:msub>
		      <m:mi>f</m:mi>
		      <m:mi>c</m:mi>
		    </m:msub></m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:apply>
	    </m:apply>
	  </m:math>
	</equation>
	Thus, 
	<equation id="eq2"> 
	  <m:math>
	    <m:apply>
	      <m:eq/>
	      <m:apply>
		<m:ci type="fn">s</m:ci>
		<m:ci>t</m:ci>
	      </m:apply>
	      <m:apply>
		<m:times/>
		<m:apply>
		  <m:plus/>
		  <m:cn>1</m:cn>
		  <m:apply>
		    <m:ci type="fn">s</m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		</m:apply>
		<m:apply>
		  <m:cos/>
		  <m:apply>
		    <m:times/>
		    <m:cn>2</m:cn>
		    <m:pi/>
		    <m:ci>
		      <m:msub>
			<m:mi>f</m:mi>
			<m:mi>c</m:mi>
		      </m:msub>
		    </m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		</m:apply>
	      </m:apply>
	      <m:apply>
		<m:plus/>
		<m:apply>
		  <m:cos/>
		  <m:apply>
		    <m:times/>
		    <m:cn>2</m:cn>
		    <m:pi/>
		    <m:ci>
		      <m:msub>
			<m:mi>f</m:mi>
			<m:mi>c</m:mi>
		      </m:msub>
		    </m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		</m:apply>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:ci type="fn">s</m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:cos/>
		    <m:apply>
		      <m:times/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		      <m:ci>
			<m:msub>
			  <m:mi>f</m:mi>
			  <m:mi>c</m:mi>
			</m:msub>
		      </m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>	      
		</m:apply>
	      </m:apply>
	    </m:apply>
	  </m:math>
	</equation>
	For the spectrum of

	<m:math>
	  <m:apply>
	    <m:cos/>
	    <m:apply>
	      <m:times/>
	      <m:cn>2</m:cn>
	      <m:pi/>
	      <m:ci>
		<m:msub>
		  <m:mi>f</m:mi>
		  <m:mi>c</m:mi>
		</m:msub>
	      </m:ci>
	      <m:ci>t</m:ci>
	    </m:apply>
	  </m:apply>
	</m:math>
	, we use the Fourier series.  Its period is 
	<m:math>
	  <m:apply>
	    <m:divide/>
	    <m:cn>1</m:cn>
	    <m:ci>
	      <m:msub>
		<m:mi>f</m:mi>
		<m:mi>c</m:mi>
	      </m:msub>
	    </m:ci>
	  </m:apply>
	</m:math>
	, and  its  only  nonzero  Fourier  coefficients  are   
	<m:math>
	  <m:apply>
	    <m:eq/>
	    <m:ci>
	      <m:msub>
		<m:mi>c</m:mi>
		<m:mrow>
		  <m:mo>±</m:mo>
		  <m:mn>1</m:mn>
		</m:mrow>
	      </m:msub>
	    </m:ci>
	    <m:apply>
	      <m:divide/>
	      <m:cn>1</m:cn>
	      <m:cn>2</m:cn>
	    </m:apply>
	  </m:apply>
	</m:math>.

	<note type="footnote">
	  From Euler's relation,   

	  <m:math>
	    <m:apply>
	      <m:eq/>
	      <m:apply>
		<m:cos/>
		<m:apply>
		  <m:times/>
		  <m:cn>2</m:cn>
		  <m:pi/>
		  <m:ci>
		    <m:msub>
		      <m:mi>f</m:mi>
		      <m:mi>c</m:mi>
		    </m:msub>
		  </m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:apply>
	      <m:apply>
		<m:plus/>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:divide/>
		    <m:cn>1</m:cn>
		    <m:cn>2</m:cn>
		  </m:apply>
		  <m:apply>
		    <m:exp/>
		    <m:apply>
		      <m:minus/>
		      <m:apply>
			<m:times/>
			<m:cn>2</m:cn>
			<m:pi/>
			<m:ci>
			  <m:msub>
			    <m:mi>f</m:mi>
			    <m:mi>c</m:mi>
			  </m:msub>
			</m:ci>
			<m:ci>t</m:ci>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:divide/>
		    <m:cn>1</m:cn>
		    <m:cn>2</m:cn>
		  </m:apply>
		  <m:apply>
		    <m:exp/>
		    <m:apply>
		      <m:times/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		      <m:ci>
			<m:msub>
			  <m:mi>f</m:mi>
			  <m:mi>c</m:mi>
			</m:msub>
		      </m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:apply>
	  </m:math>.
	  This is the Fourier series for cosine!
	</note> 


	The second term is <emphasis>not </emphasis>periodic unless 
	<m:math>
	  <m:apply>
	    <m:ci type="fn">s</m:ci>
	    <m:ci>t</m:ci>
	  </m:apply>
	</m:math>
	has the same period as the sinusoid.  Using Euler's relation,
	the spectrum of the second term can be derived as
	<equation id="eq3">
	  <m:math>
	    <m:apply>
	      <m:eq/>
	      <m:apply>
		<m:times/>
		<m:apply>
		  <m:ci type="fn">s</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
		<m:apply>
		  <m:cos/>
		  <m:apply>
		    <m:times/>
		    <m:cn>2</m:cn>
		    <m:pi/>
		    <m:ci>
		      <m:msub>
			<m:mi>f</m:mi>
			<m:mi>c</m:mi>
		      </m:msub>
		    </m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		</m:apply>
	      </m:apply>
	      <m:apply>
		<m:times/>
		<m:apply>
		  <m:int/>
		  <m:bvar><m:ci>f</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:times/>
		    <m:apply>
		      <m:ci type="fn">S</m:ci>
		      <m:ci>f</m:ci>
		    </m:apply>
		    <m:apply>
		      <m:exp/>
		      <m:apply>
			<m:times/>
			<m:imaginaryi/>
			<m:cn>2</m:cn>
			<m:pi/>
			<m:ci>f</m:ci>
			<m:ci>t</m:ci>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
		<m:apply>
		  <m:cos/>
		  <m:apply>
		    <m:times/>
		    <m:cn>2</m:cn>
		    <m:pi/>
		    <m:ci>
		      <m:msub>
			<m:mi>f</m:mi>
			<m:mi>c</m:mi>
		      </m:msub>
		    </m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		</m:apply>
	      </m:apply>
	      
	      <m:apply>
		<m:plus/>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:divide/>
		    <m:cn>1</m:cn>
		    <m:cn>2</m:cn>
		  </m:apply>
		  <m:apply>
		    <m:int/>
		    <m:bvar><m:ci>f</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:times/>
		      <m:apply>
			<m:ci type="fn">S</m:ci>
			<m:ci>f</m:ci>
		      </m:apply>
		      <m:apply>
			<m:exp/>
			<m:apply>
			  <m:times/>
			  <m:imaginaryi/>
			  <m:cn>2</m:cn>
			  <m:pi/>
			  <m:apply>
			    <m:plus/>
			    <m:ci>f</m:ci>
			    <m:ci>
			      <m:msub>
				<m:mi>f</m:mi>
				<m:mi>c</m:mi>
			      </m:msub>
			    </m:ci>			
			  </m:apply>
			  <m:ci>t</m:ci>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:divide/>
		    <m:cn>1</m:cn>
		    <m:cn>2</m:cn>
		  </m:apply>
		  <m:apply>
		    <m:int/>
		    <m:bvar><m:ci>f</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:times/>
		      <m:apply>
			<m:ci type="fn">S</m:ci>
			<m:ci>f</m:ci>
		      </m:apply>
		      <m:apply>
			<m:exp/>
			<m:apply>
			  <m:times/>
			  <m:imaginaryi/>
			  <m:cn>2</m:cn>
			  <m:pi/>
			  <m:apply>
			    <m:minus/>
			    <m:ci>f</m:ci>
			    <m:ci>
			      <m:msub>
				<m:mi>f</m:mi>
				<m:mi>c</m:mi>
			      </m:msub>
			    </m:ci>			
			  </m:apply>
			  <m:ci>t</m:ci>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>

	      <m:apply>
		<m:plus/>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:divide/>
		    <m:cn>1</m:cn>
		    <m:cn>2</m:cn>
		  </m:apply>
		  <m:apply>
		    <m:int/>
		    <m:bvar><m:ci>f</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:times/>
		      <m:apply>
			<m:ci type="fn">S</m:ci>
			<m:apply>
			  <m:minus/>
			  <m:ci>f</m:ci>
			  <m:ci>
			    <m:msub>
			      <m:mi>f</m:mi>
			      <m:mi>c</m:mi>
			    </m:msub>
			  </m:ci>			
			</m:apply>
		      </m:apply>
		      <m:apply>
			<m:exp/>
			<m:apply>
			  <m:times/>
			  <m:imaginaryi/>
			  <m:cn>2</m:cn>
			  <m:pi/>
			  <m:ci>f</m:ci>
			  <m:ci>t</m:ci>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:divide/>
		    <m:cn>1</m:cn>
		    <m:cn>2</m:cn>
		  </m:apply>
		  <m:apply>
		    <m:int/>
		    <m:bvar><m:ci>f</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:times/>
		      <m:apply>
			<m:ci type="fn">S</m:ci>
			<m:apply>
			  <m:plus/>
			  <m:ci>f</m:ci>
			  <m:ci>
			    <m:msub>
			      <m:mi>f</m:mi>
			      <m:mi>c</m:mi>
			    </m:msub>
			  </m:ci>			
			</m:apply>
		      </m:apply>
		      <m:apply>
			<m:exp/>
			<m:apply>
			  <m:times/>
			  <m:imaginaryi/>
			  <m:cn>2</m:cn>
			  <m:pi/>
			  <m:ci>f</m:ci>
			  <m:ci>t</m:ci>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>

	      <m:apply>
		<m:int/>
		<m:bvar><m:ci>f</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:times/>
		  <m:apply>
		    <m:divide/>
		    <m:apply>
		      <m:plus/>
		      <m:apply>
			<m:ci type="fn">S</m:ci>
			<m:apply>
			  <m:minus/>
			  <m:ci>f</m:ci>
			  <m:ci>
			    <m:msub>
			      <m:mi>f</m:mi>
			      <m:mi>c</m:mi>
			    </m:msub>
			  </m:ci>			
			</m:apply>
		      </m:apply>
		      <m:apply>
			<m:ci type="fn">S</m:ci>
			<m:apply>
			  <m:plus/>
			  <m:ci>f</m:ci>
			  <m:ci>
			    <m:msub>
			      <m:mi>f</m:mi>
			      <m:mi>c</m:mi>
			    </m:msub>
			  </m:ci>			
			</m:apply>
		      </m:apply>
		    </m:apply>
		    <m:cn>2</m:cn>
		  </m:apply>
		  <m:apply>
		    <m:exp/>
		    <m:apply>
		      <m:times/>
		      <m:imaginaryi/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		      <m:ci>f</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:apply>
	  </m:math>
	</equation>      

	
	Exploiting the uniqueness property of the Fourier transform, we have  

	<equation id="eq7">
	  <m:math>
	    <m:apply>
	      <m:eq/>
	      <m:apply>
		<m:ci type="fn">F</m:ci>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:ci type="fn">s</m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:cos/>
		    <m:apply>
		      <m:times/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		      <m:ci>
			<m:msub>
			  <m:mi>f</m:mi>
			  <m:mi>c</m:mi>
			</m:msub>
		      </m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>

	      <m:apply>
		<m:divide/>
		<m:apply>
		  <m:plus/>
		  <m:apply>
		    <m:ci type="fn">S</m:ci>
		    <m:apply>
		      <m:minus/>
		      <m:ci>f</m:ci>
		      <m:ci>
			<m:msub>
			  <m:mi>f</m:mi>
			  <m:mi>c</m:mi>
			</m:msub>
		      </m:ci>			
		    </m:apply>
		  </m:apply>
		  <m:apply>
		    <m:ci type="fn">S</m:ci>
		    <m:apply>
		      <m:plus/>
		      <m:ci>f</m:ci>
		      <m:ci>
			<m:msub>
			  <m:mi>f</m:mi>
			  <m:mi>c</m:mi>
			</m:msub>
		      </m:ci>			
		    </m:apply>
		  </m:apply>
		</m:apply>
		<m:cn>2</m:cn>
	      </m:apply>
	    </m:apply>
	  </m:math>
	</equation>

	This component of the spectrum consists of the original
	signal's spectrum delayed and advanced <emphasis>in
	  frequency</emphasis>.  The spectrum of the amplitude modulated
	signal is shown in <cnxn target="modulated" strength="7"/>.
      </para>

      <figure id="modulated">
	<name>modulated</name> <media type="image/png" src="spectrum5.png"/> <caption>A signal which has a triangular
	  shaped spectrum is shown in the top plot.  Its highest
	  frequency—the largest frequency containing
	  power—is <m:math>
	    <m:ci>W</m:ci>
	  </m:math>
	   Hz.  Once amplitude modulated, the resulting spectrum
	  has "lines" corresponding to the Fourier series components
	  at <m:math>
	    <m:apply>
	      <m:mo>±</m:mo>
	      <m:ci>
		<m:msub>
		  <m:mi>f</m:mi>
		  <m:mi>c</m:mi>
		</m:msub>
	      </m:ci>
	    </m:apply>
	  </m:math>
	  and the original triangular spectrum shifted to components
	  at
	  <m:math>
	    <m:apply>
	      <m:mo>±</m:mo>
	      <m:ci>
		<m:msub>	
		  <m:mi>f</m:mi>	
		  <m:mi>c</m:mi>	
		</m:msub>	
	      </m:ci>	
	    </m:apply>	
	  </m:math> 
	  and scaled by   
	  <m:math>
	    <m:apply>
	      <m:divide/>
	      <m:cn>1</m:cn>	
	      <m:cn>2</m:cn>
	    </m:apply>
	  </m:math>.
	</caption>
      </figure>

      <para id="MoreFreqDomain">
	Note how in this figure the signal   
	<m:math>         
	  <m:apply>
	    <m:ci type="fn">s</m:ci>
	    <m:ci>t</m:ci>
	  </m:apply>      
	</m:math>
	is defined in the frequency domain. To find its time domain
	representation, we simply use the inverse Fourier transform.
      </para>
    </example>

    <exercise id="ex1">
      <problem>
	<para id="ex1a">What is the signal
	  <m:math>         
	    <m:apply>
	      <m:ci type="fn">s</m:ci>
	      <m:ci>t</m:ci>
	    </m:apply>      
	  </m:math>
	  that corresponds to the spectrum shown in the upper panel of
	  <cnxn target="modulated" strength="8"/>?
	</para>
      </problem>
      <solution>
	<para id="ex1b"> The signal is the inverse Fourier transform
	  of the triangularly shaped spectrum, and equals
	  <m:math>
	    <m:apply>
	      <m:eq/>
	      <m:apply>
		<m:ci type="fn">s</m:ci>
		<m:ci>t</m:ci>
	      </m:apply>
	      <m:apply>
		<m:times/>
		<m:ci>W</m:ci>
		<m:apply>
		  <m:power/>
		  <m:apply>
		    <m:divide/>
		    <m:apply>
		      <m:sin/>
		      <m:apply>
			<m:times/>
			<m:pi/>
			<m:ci>W</m:ci>
			<m:ci>t</m:ci>
		      </m:apply>
		    </m:apply>
		    <m:apply>
		      <m:times/>
		      <m:pi/>
		      <m:ci>W</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		  <m:cn>2</m:cn>
		</m:apply>
	      </m:apply>
	    </m:apply>      
	  </m:math>                                                              
	</para>        
      </solution>
    </exercise>

    <exercise id="ex2">
      <problem>
	<para id="ex2a">
	  What is the power in 
	  <m:math>         
	    <m:apply>
	      <m:ci type="fn">x</m:ci>
	      <m:ci>t</m:ci>
	    </m:apply>      
	  </m:math>
	  , the amplitude-modulated signal?  Try the calculation in
	  both the time and frequency domains.
	</para>
      </problem>
      <solution>
	<para id="ex2b">
	  The result is most easily found in the spectrum's formula:
	  the power in the signal-related part of <m:math>
	    <m:apply>
	      <m:ci type="fn">x</m:ci>
	      <m:ci>t</m:ci>
	    </m:apply>      
	  </m:math>
	  is half the power of the signal   
	  <m:math>         
	    <m:apply>
	      <m:ci type="fn">s</m:ci>
	      <m:ci>t</m:ci>
	    </m:apply>      
	  </m:math>.
	</para>
      </solution>
    </exercise>

    <para id="baseband">   In this example, we call the signal   
      <m:math>         
	<m:apply>
	  <m:ci type="fn">s</m:ci>
	  <m:ci>t</m:ci>
	</m:apply>      
      </m:math>
      a <term>baseband signal </term>because its power is contained at
      low frequencies. Signals such as speech and the Dow Jones
      averages are baseband signals.  The baseband signal's
      <term>bandwidth </term>equals
      <m:math>
	<m:apply>
	  <m:ci>W</m:ci>
	</m:apply>      
      </m:math>
      , the highest frequency at which it has power.  Since
      <m:math>         
	<m:apply>
	  <m:ci type="fn">x</m:ci>
	  <m:ci>t</m:ci>
	</m:apply>      
      </m:math>
      's spectrum is confined to a frequency band not close to the
      origin (we assume
      <m:math>
	<m:apply>
	  <m:mo>≫</m:mo>
	  <m:ci><m:msub>	
	      <m:mi>f</m:mi>	
	      <m:mi>c</m:mi>	
	    </m:msub></m:ci>	
	  <m:ci>W</m:ci>
	</m:apply>
      </m:math>
      ), we have a <term>bandpass signal</term>.  The bandwidth of a
      bandpass signal is <emphasis>not </emphasis>its highest
      frequency, but the range of positive frequencies where the
      signal has power.  Thus, in this example, the bandwidth is
      <m:math>
	<m:apply>
	  <m:times/>
	  <m:cn>2</m:cn>
	  <m:ci>W</m:ci>
	</m:apply>
	<m:ci>Hz</m:ci> </m:math>.  Why a signal's bandwidth should
      depend on its spectral shape will become clear once we develop
      communications systems.
    </para>

  </content>
</document>
