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<document xmlns="http://cnx.rice.edu/cnxml" xmlns:q="http://cnx.rice.edu/qml/1.0" 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="m10350"> 

  <name>Frequency Domain Problems</name>
  <metadata>
  <md:version>2.31</md:version>
  <md:created>2001/08/22</md:created>
  <md:revised>2008/07/06 16:23:21.541 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="bfite">
      <md:firstname>Benjamin</md:firstname>
      
      <md:surname>Fite</md:surname>
      <md:email>bfite@rice.edu</md:email>
    </md:maintainer>
    <md:maintainer id="brentmh">
      <md:firstname>Brent</md:firstname>
      <md:othername>Michael</md:othername>
      <md:surname>Hendricks</md:surname>
      <md:email>brentmh@rice.edu</md:email>
    </md:maintainer>
    <md:maintainer id="jsilv">
      <md:firstname>Jeffrey</md:firstname>
      <md:othername>M</md:othername>
      <md:surname>Silverman</md:surname>
      <md:email>JSilverman@astro.berkeley.edu</md:email>
    </md:maintainer>
    <md:maintainer id="ernsnave">
      <md:firstname>Erin</md:firstname>
      
      <md:surname>Snavely</md:surname>
      <md:email>ernsnave@alumni.rice.edu</md:email>
    </md:maintainer>
  </md:maintainerlist>
  
  

  <md:abstract>Problems dealing with Fourier Series.</md:abstract>
</metadata>

  <content>
    
    <q:problemset>  
      
      <q:item id="i4.1a" type="text-response"> <!--problem 1a -->
        <q:question>
	    <section id="s1a">
	    <name>Simple Fourier Series</name>
	    <para id="p4.1a">
	      Find the complex Fourier series representations of the following signals without explicitly calculating Fourier integrals.
	      What is the signal's period in each case?
	    </para>

	    <list id="list4.1a" type="enumerated">
	      <item>
		   <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:sin/><m:ci>t</m:ci></m:apply>
		     </m:apply>
		   </m:math>
	      </item>
	      
	      <item>
		   <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:power/>
		         <m:apply><m:sin/><m:ci>t</m:ci></m:apply>
		         <m:cn>2</m:cn>
		       </m:apply>
		     </m:apply>
		   </m:math>
	      </item>
	      
	      <item>
	        <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:plus/>
		         <m:apply><m:cos/><m:ci>t</m:ci></m:apply>
		         <m:apply><m:times/>
		           <m:cn>2</m:cn>
		           <m:apply><m:cos/>
		             <m:apply><m:times/>
		               <m:cn>2</m:cn>
		               <m:ci>t</m:ci>
                     </m:apply>
                   </m:apply>
		         </m:apply>
		       </m:apply>
		     </m:apply>
	        </m:math>
	      </item>

	      <item>
	        <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:cos/>
		           <m:apply><m:times/>
		             <m:cn>2</m:cn>
		             <m:ci>t</m:ci>
                   </m:apply>
                 </m:apply>
		         <m:apply><m:cos/><m:ci>t</m:ci></m:apply>
		       </m:apply>
		     </m:apply>
		   </m:math>
	      </item>
	      
	      <item>
	        <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:cos/>
		           <m:apply><m:plus/>
		             <m:apply><m:times/>
		               <m:cn>10</m:cn>
		               <m:pi/>
		               <m:ci>t</m:ci>
		             </m:apply>
		             <m:apply><m:divide/>
		               <m:pi/>
		               <m:cn>6</m:cn>
		             </m:apply>
                   </m:apply>
                 </m:apply>
                 <m:apply><m:plus/>
                   <m:cn>1</m:cn>
                   <m:apply><m:cos/>
                     <m:apply><m:times/>
                       <m:cn>2</m:cn>
                       <m:pi/>
                       <m:ci>t</m:ci>
                     </m:apply>
                   </m:apply>
                 </m:apply>
		       </m:apply>
		     </m:apply>
		   </m:math>
	      </item>
	      
	      <item>
	        <m:math>
	          <m:apply><m:ci type="fn">s</m:ci><m:ci>t</m:ci></m:apply>
	        </m:math> given by the depicted
	        <cnxn target="fig4.1a">waveform</cnxn>.
	        <figure orient="vertical" id="fig4.1a">
	          <media type="image/png" src="sig52.png"/>
	        </figure>
	      </item>

	    </list>
	    </section>
	    </q:question>	
      </q:item>

      <q:item id="i1" type="text-response"> <!--problem 1 -->
        <q:question>
	  <section id="sec1">
	    <name>Fourier Series</name>
	    <para id="p4.1">
	      Find the Fourier series representation for the <cnxn target="fig4.1" strength="9">following periodic
	      signals</cnxn>. For the third signal, find the complex
	      Fourier series for the triangle wave
	      <emphasis>without</emphasis> performing the usual
	      Fourier integrals. Hint: How is this signal related to
	      one for which you already have the series?
	    </para>


	    <figure orient="vertical" id="fig4.1">
	      <subfigure>		
		<media type="image/png" src="sig6.png"/>
	      </subfigure>
	      <subfigure>		
		<media type="image/png" src="sig7.png"/>
	      </subfigure>
	      <subfigure>		
		<media type="image/png" src="sig8.png"/>
	      </subfigure>
	    </figure>
	    
	  </section>
	</q:question>	
      </q:item>


      <q:item id="i4.2" type="text-response"> <!--problem 2 -->
        <q:question>
	  <section id="s2">
	    <name>Phase Distortion</name>
	    <para id="p4.2">
	      We can learn about phase distortion by returning to
	      circuits and investigate the
             <cnxn target="fig4.2" strength="9">following circuit</cnxn>.
	    </para>

	    <figure id="fig4.2">
	      <media type="image/png" src="circuit3.png"/>
	    </figure>

	    <list id="list4.2" type="enumerated">
	      <item>
		Find this filter's transfer function.
	      </item>
	      <item>
		Find the magnitude and phase of this transfer
		function. How would you characterize this
		circuit?
	      </item> 
	      <item>
		Let
		<m:math>
		  <m:apply>
		    <m:ci type="fn">
		      <m:msub>
			<m:mi>v</m:mi>
			<m:mi>in</m:mi>
		      </m:msub>
		    </m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		</m:math>
		be a square-wave of period
		<m:math>
		  <m:ci>T</m:ci>
		</m:math>. 
		What is the Fourier series for the output voltage?
	      </item>
	      <item>
		Use Matlab to find the output's waveform for the cases
		<m:math>
		  <m:apply>
		    <m:eq/>
		    <m:ci>T</m:ci>
		    <m:cn>0.01</m:cn>
		  </m:apply>
		</m:math>
		and
		<m:math>
		  <m:apply>
		    <m:eq/>
		    <m:ci>T</m:ci>
		    <m:cn>2</m:cn>
		  </m:apply>
		</m:math>.		
		What value of
		<m:math>
		  <m:ci>T</m:ci>
		</m:math>
		delineates the two kinds of results you found? The
		software in <code>fourier2.m</code> might be
		useful.
	      </item>	      
	      <item>
		Instead of the depicted circuit, the square wave is
		passed through a system that delays its input, which
		applies a linear phase shift to the signal's
		spectrum. Let the delay
		<m:math><m:ci>τ</m:ci></m:math> be
		<m:math>
		  <m:apply>
		    <m:divide/>
		    <m:ci>T</m:ci>
		    <m:cn>4</m:cn>
		  </m:apply>
		</m:math>.  
		Use the transfer function of a delay to compute using
		Matlab the Fourier series of the output. Show that the
		square wave is indeed delayed.
	      </item>	      
	    </list>
	  </section>
	</q:question>	
      </q:item>

      
      <q:item id="i3" type="text-response"> <!--problem 3 -->
        <q:question>
	  <section id="s4.3">
	    <name>Approximating Periodic Signals</name>
	    <para id="p4.3">
	      Often, we want to approximate a reference signal by a
	      somewhat simpler signal. To assess the quality of an
	      approximation, the most frequently used error measure is
	      the mean-squared error. For a periodic signal
	      <m:math>
		<m:apply>
		  <m:ci type="fn">s</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>,
	      
	      <m:math display="block">
		<m:apply>
		  <m:eq/>
		  <m:apply>
		    <m:power/>
		    <m:ci>ε</m:ci>
		    <m:cn>2</m:cn>
		  </m:apply>
		  <m:apply>
		    <m:times/>
		    <m:apply>
		      <m:divide/>
		      <m:cn>1</m:cn>
		      <m:ci>T</m:ci>
		    </m:apply>
		    <m:apply>
		      <m:int/>
		      <m:bvar>
			<m:ci>t</m:ci>
		      </m:bvar>
		      <m:lowlimit>
			<m:cn>0</m:cn>
		      </m:lowlimit>
		      <m:uplimit>
			<m:ci>T</m:ci>
		      </m:uplimit>    
		      <m:apply>
			<m:power/>
			<m:apply>
			  <m:minus/>
			  <m:apply>
			    <m:ci type="fn">s</m:ci>
			    <m:ci>t</m:ci>
			  </m:apply>
			  <m:apply>
			    <m:ci type="fn">
			      <m:mover>
				<m:mi>s</m:mi>
				<m:mo>˜</m:mo>
			      </m:mover>
			    </m:ci>
			    <m:ci>t</m:ci>
			  </m:apply>
			</m:apply>
			<m:cn>2</m:cn>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:math>
	      
	      where	      
	      <m:math>
		<m:apply>
		  <m:ci type="fn">s</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>	      
	      is the reference signal and 	      
	      <m:math>
		<m:apply>
		  <m:ci type="fn">
		    <m:mover>
		      <m:mi>s</m:mi>
		      <m:mo>˜</m:mo>
		    </m:mover>
		  </m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>	      
	      its approximation. One convenient way of finding
	      approximations for periodic signals is to truncate their
	      Fourier series.
	      
	      <m:math display="block">
		<m:apply>
		  <m:eq/>
		  <m:apply>
		    <m:ci type="fn">
		      <m:mover>
			<m:mi>s</m:mi>
			<m:mo>˜</m:mo>
		      </m:mover>
		    </m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:sum/>
		    <m:bvar>
		      <m:ci>k</m:ci>
		    </m:bvar>
		    <m:lowlimit>
		      <m:apply>
			<m:minus/>
			<m:ci>K</m:ci>
		      </m:apply>
		    </m:lowlimit>
		    <m:uplimit>
		      <m:ci>K</m:ci>
		    </m:uplimit>
		    <m:apply>
		      <m:times/>
		      <m:ci>
			<m:msub>
			  <m:mi>c</m:mi>
			  <m:mi>k</m:mi>
			</m:msub>
		      </m:ci>
		      <m:apply>
			<m:exp/>
			<m:apply>
			  <m:times/>
			  <m:imaginaryi/>
			  <m:apply>
			    <m:divide/>
			    <m:apply>
			      <m:times/>
			      <m:cn>2</m:cn>
			      <m:pi/>
			      <m:ci>k</m:ci>
			    </m:apply>
			    <m:ci>T</m:ci>
			  </m:apply>
			  <m:ci>t</m:ci>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:math>
	      
	      The point of this problem is to analyze whether this
	      approach is the best (<foreign>i.e.</foreign>, always
	      minimizes the mean-squared error).
	      
	      <list id="list4.3" type="enumerated">
		<item>
		  Find a frequency-domain expression for the
		  approximation error when we use the truncated
		  Fourier series as the approximation.
		</item>
		<item>
		  Instead of truncating the series, let's generalize
		  the nature of the approximation to including any set
		  of
		  <m:math>
		    <m:apply>
		      <m:plus/>
		      <m:apply>
			<m:times/>
			<m:cn>2</m:cn>
			<m:ci>K</m:ci>  
		      </m:apply>
		      <m:cn>1</m:cn>
		    </m:apply>
		  </m:math>		  
		  terms: We'll always include the		  
		  <m:math>
		    <m:ci>
		      <m:msub>
			<m:mi>c</m:mi>
			<m:mn>0</m:mn>
		      </m:msub>
		    </m:ci>
		  </m:math>
		  and the negative indexed term corresponding to
		  <m:math>
		    <m:ci>
		      <m:msub>
			<m:mi>c</m:mi>
			<m:mi>k</m:mi>
		      </m:msub>
		    </m:ci>
		  </m:math>.
		  What selection of terms minimizes the mean-squared
		  error? Find an expression for the mean-squared error
		  resulting from your choice.
		</item>		
		<item>
		  Find the Fourier series for the
           <cnxn target="fig4.3.bubba" strength="9">depicted signal</cnxn>. Use
		  Matlab to find the truncated approximation and best
		  approximation involving two terms. Plot the
		  mean-squared error as a function of
		  <m:math><m:ci>K</m:ci></m:math> for both
		  approximations.
		</item>
	      </list>
	    </para>
	    
	    <figure id="fig4.3.bubba">
	      <media type="image/png" src="sig9.png"/>
	    </figure>
	    
	  </section>
	</q:question>	
      </q:item>


      <q:item id="i4" type="text-response"> <!--problem 4 -->
        <q:question>
	  <section id="s4">
	    <name>Long, Hot Days</name>
	    <para id="p4.4">
	      The daily temperature is a consequence of several
	      effects, one of them being the sun's heating. If this
	      were the dominant effect, then daily temperatures would
	      be proportional to the number of daylight hours. The
	      <cnxn target="fig4.4" strength="9">plot</cnxn> shows
	      that the average daily high temperature does
	      <emphasis>not</emphasis> behave that way.
	    </para>

	    <figure id="fig4.4">
	      <media type="image/png" src="sig38.png"/>
	    </figure>

	    <para id="p4.4cyclomethicone">
	      In this problem, we want to understand the temperature
	      component of our environment using Fourier series and
	      linear system theory. The file
	      <code>temperature.mat</code> contains these data
	      (daylight hours in the first row, corresponding average
	      daily highs in the second) for Houston, Texas.

	      <list id="list4.4" type="enumerated">
		<item>
		  Let the length of day serve as the sole input to a
		  system having an output equal to the average daily
		  temperature. Examining the plots of input and
		  output, would you say that the system is linear or
		  not? How did you reach you conclusion?
		</item>
		<item>
		  Find the first five terms
		  (<m:math display="inline">
		    <m:apply>
		      <m:ci>
			<m:msub>
			  <m:mi>c</m:mi>
			  <m:mn>0</m:mn>
			</m:msub>
		      </m:ci>
		    </m:apply>
		  </m:math>,
		  ... ,		  
		  <m:math>
		    <m:apply>
		      <m:ci>
			<m:msub>
			  <m:mi>c</m:mi>
			  <m:mn>4</m:mn>
			</m:msub>
		      </m:ci>
		    </m:apply>
		  </m:math>) 
		  of the complex Fourier series for each signal.
		</item>
		<item>
		  What is the harmonic distortion in the two signals?
		  Exclude
		  <m:math>
		    <m:apply>
		      <m:ci>
			<m:msub>
			  <m:mi>c</m:mi>
			  <m:mn>0</m:mn>
			</m:msub>
		      </m:ci>
		    </m:apply>
		  </m:math>
		  from this calculation.
		</item>
		<item>
		  Because the harmonic distortion is small, let's
		  concentrate only on the first harmonic. What is the
		  phase shift between input and output signals?
		</item>
		<item>
		  Find the transfer function of the simplest possible
		  linear model that would describe the data.
		  Characterize and interpret the structure of this
		  model. In particular, give a physical explanation
		  for the phase shift.
		</item>
		<item>
		  Predict what the output would be if the model had no
		  phase shift. Would days be hotter? If so, by how
		  much?
		</item>		
	      </list>
	    </para>
	  </section>
	</q:question>	
      </q:item>

      
      <q:item id="i5" type="text-response"> <!--problem 5 -->
        <q:question>
	  <section id="s5">
	    <name>Fourier Transform Pairs</name>
	    <para id="p5">
	      Find the Fourier or inverse Fourier transform of the
	      following.

	      <list id="list4.5" type="enumerated">
		<item>
		  <m:math>
		    <m:apply>
		      <m:forall/>
		      <m:bvar>
			<m:ci>t</m:ci>
		      </m:bvar>
		      <m:condition>
			<m:apply>
			  <m:lt/>
			  <m:apply>
			    <m:minus/>
			    <m:infinity/>
			  </m:apply>
			  <m:ci>t</m:ci>
			  <m:infinity/>
			</m:apply>
		      </m:condition>
		      <m:apply>
			<m:eq/>
			<m:apply>
			  <m:ci type="fn">x</m:ci>
			  <m:ci>t</m:ci>
			</m:apply>
			<m:apply>
			  <m:exp/>
			  <m:apply>
			    <m:minus/>
			    <m:apply>
			      <m:times/>			  
			      <m:ci>a</m:ci>
			      <m:apply>
				<m:abs/>
				<m:ci>t</m:ci>
			      </m:apply>
			    </m:apply>
			  </m:apply>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:math>
		</item>		

		<item>
		  <m:math>
		    <m:apply>
		      <m:eq/>
		      <m:apply>
			<m:ci type="fn">x</m:ci>
			<m:ci>t</m:ci>
		      </m:apply>
		      <m:apply>
			<m:times/>
			<m:ci>t</m:ci>
			<m:apply>
			  <m:exp/>
			  <m:apply>
			    <m:minus/>
			    <m:apply><m:times/>
				<m:ci>a</m:ci>
			        <m:ci>t</m:ci>
			    </m:apply>
			  </m:apply>
			</m:apply>
			<m:apply>
			  <m:ci type="fn">u</m:ci>
			  <m:ci>t</m:ci>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:math>
		</item>		
		<item>
		  <m:math>
		    <m:apply>
		      <m:eq/>
		      <m:apply>
			<m:ci type="fn">X</m:ci>
			<m:ci>f</m:ci>
		      </m:apply>
		      <m:piecewise>
			<m:piece>
			  <m:cn>1</m:cn>
			  <m:apply>
			    <m:lt/>
			    <m:apply>
			      <m:abs/>
			      <m:ci>f</m:ci>
			    </m:apply>
			    <m:ci>W</m:ci>
			  </m:apply>
			</m:piece>
			<m:piece>
			  <m:cn>0</m:cn>
			  <m:apply>
			    <m:gt/>
			    <m:apply>
			      <m:abs/>
			      <m:ci>f</m:ci>
			    </m:apply>
			    <m:ci>W</m:ci>
			  </m:apply>
			</m:piece>
		      </m:piecewise>
		    </m:apply>
		  </m:math>
		</item>		
		<item>
		  <m:math>
		    <m:apply>
		      <m:eq/>
		      <m:apply>
			<m:ci type="fn">x</m:ci>
			<m:ci>t</m:ci>
		      </m:apply>
		      <m:apply>
			<m:times/>
			<m:apply>
			  <m:exp/>
			  <m:apply>
			    <m:minus/>
			    <m:apply>
			      <m:times/>
			      <m:ci>a</m:ci>
			      <m:ci>t</m:ci>
			    </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:mn>0</m:mn>
			      </m:msub>
			    </m:ci>
			    <m:ci>t</m:ci>
			  </m:apply>
			</m:apply>
			<m:apply>
			  <m:ci type="fn">u</m:ci>
			  <m:ci>t</m:ci>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:math>
		</item>		
	      </list>
	    </para>
	  </section>
	</q:question>	
      </q:item>

      <q:item id="i4.5a" type="text-response"> <!--problem 5a -->
        <q:question>
	    <section id="s5a">
	    <name>Duality in Fourier Transforms</name>
	    <para id="p4.5a">
	      "Duality" means that the Fourier transform and the inverse Fourier transform are very similar.
	      Consequently, the waveform
	      <m:math>
	        <m:apply><m:ci type="fn">s</m:ci><m:ci>t</m:ci></m:apply>
	      </m:math>
	      in the time domain and the spectrum
	      <m:math>
	        <m:apply><m:ci type="fn">s</m:ci><m:ci>f</m:ci></m:apply>
	      </m:math>
	      have a Fourier transform and an inverse Fourier transform, respectively, that are very similar.
	    </para>
	    
	    <list id="p4.5aparts" type="enumerated">
	      <item>
	        Calculate the Fourier transform of the signal shown
	        <cnxn target="fig4.5a1">below</cnxn>.
	      </item>
	      <item>
	        Calculate the inverse Fourier transform of the spectrum shown
	        <cnxn target="fig4.5a2">below</cnxn>.
	      </item>
	      <item>
	        How are these answers related?
	        What is the general relationship between the Fourier transform of
	        <m:math>
	          <m:apply><m:ci type="fn">s</m:ci><m:ci>t</m:ci></m:apply>
	        </m:math>
	        and the inverse transform of
	      <m:math>
	        <m:apply><m:ci type="fn">s</m:ci><m:ci>f</m:ci></m:apply>
	      </m:math>?
	      </item>
	    </list>

	    <figure orient="horizontal" id="fig4.5a">
	      <subfigure id="fig4.5a1">
	        <media type="image/png" src="sig53a.png"/>
	      </subfigure>
	      <subfigure id="fig4.5a2">
	        <media type="image/png" src="sig53b.png"/>
	      </subfigure>
	    </figure>

	    </section>
	    </q:question>	
      </q:item>

      <q:item id="i4.5b" type="text-response"> <!--problem 5b -->
        <q:question>
	    <section id="s5b">
	    <name>Spectra of Pulse Sequences</name>
	    <para id="p4.5b">
	      Pulse sequences occur often in digital communication and in other fields as well.
	      What are their spectral properties?
	    </para>
	    
	    <list id="p4.5bparts" type="enumerated">
	      <item>
	        Calculate the Fourier transform of the single pulse shown
	        <cnxn target="fig4.5b1">below</cnxn>.
	      </item>
	      <item>
	        Calculate the Fourier transform of the two-pulse sequence shown
	        <cnxn target="fig4.5b2">below</cnxn>.
	      </item>
	      <item>
	        Calculate the Fourier transform for the <emphasis>ten</emphasis>-pulse sequence shown in <cnxn target="fig4.5b3">below</cnxn>.
	        You should look for a general expression that holds for sequences of any length.
	      </item>
	      <item>
	      Using Matlab, plot the magnitudes of the three spectra.
	      Describe how the spectra change as the number of repeated pulses increases.
	      </item>
	    </list>

	    <figure orient="vertical" id="fig4.5b">
	      <subfigure id="fig4.5b1">
	        <media type="image/png" src="sig54a.png"/>
	      </subfigure>
	      <subfigure id="fig4.5b2">
	        <media type="image/png" src="sig54b.png"/>
	      </subfigure>
	      <subfigure id="fig4.5b3">
	        <media type="image/png" src="sig54c.png"/>
	      </subfigure>
	    </figure>

	    </section>
	    </q:question>	
      </q:item>

      <q:item id="i6" type="text-response"> <!--problem 6 -->
        <q:question>
	  <section id="sec6">
	    <name>Lowpass Filtering a Square Wave</name>
	    <para id="p6">
	      Let a square wave (period 
	      <m:math>
		<m:ci>T</m:ci>
	      </m:math>) 
	      serve as the input to a first-order lowpass system
	      constructed as a RC filter.  We want to derive an
	      expression for the time-domain response of the filter to
	      this input.

	      <list id="list4.6" type="enumerated">
		<item>
		  First, consider the response of the filter to a
		  simple pulse, having unit amplitude and width
		  <m:math>
		    <m:apply>
		      <m:divide/>
		      <m:ci>T</m:ci>
		      <m:cn>2</m:cn>
		    </m:apply>
		  </m:math>.
		  Derive an expression for the filter's output to this
		  pulse.
		</item>	
		
		<item>
		  Noting that the square wave is a superposition of a
		  sequence of these pulses, what is the filter's
		  response to the square wave?
		</item>	
		
		<item>
		  The nature of this response should change as the
		  relation between the square wave's period and the
		  filter's cutoff frequency change.  How long must the
		  period be so that the response does
		  <emphasis>not</emphasis> achieve a relatively
		  constant value between transitions in the square
		  wave?  What is the relation of the filter's cutoff
		  frequency to the square wave's spectrum in this
		  case?
		</item>
		
	      </list>
	    </para>
	  </section>
	</q:question>	
      </q:item>


      <q:item id="i7" type="text-response"> <!--problem 7 -->
        <q:question>
	  <section id="s7">
	    <name>Mathematics with Circuits</name>
	    <para id="p7">
	      Simple circuits can implement simple mathematical
	      operations, such as integration and differentiation. We
	      want to develop an active circuit (it contains an
	      op-amp) having an output that is proportional to the
	      integral of its input.  For example, you could use an
	      integrator in a car to determine distance traveled from
	      the speedometer.

	      <list id="list4.7" type="enumerated">
		<item>
		  What is the transfer function of an integrator?
		</item>
		<item>
		  Find an op-amp circuit so that its voltage output is
		  proportional to the integral of its input for all
		  signals.
		</item>		
	      </list>
	    </para>
	  </section>
	</q:question>	
      </q:item>

      
      <q:item id="i8" type="text-response"> <!--problem 8 -->
        <q:question>
	  <section id="s8">
	    <name>Where is that sound coming from? </name>
	    <para id="p8">
	      We determine where sound is coming from because we have
	      two ears and a brain.  Sound travels at a relatively
	      slow speed and our brain uses the fact that sound will
	      arrive at one ear before the other.  <cnxn target="fig4.8" strength="9">As shown here</cnxn>, a
	      sound coming from the right arrives at the left ear
	      <m:math><m:ci>τ</m:ci></m:math> seconds after it
	      arrives at the right ear.
	    </para>
	    
	    <figure id="fig4.8">
	      <media type="image/png" src="sound.png"/>
	    </figure>

	    <para id="p8.2">
	      Once the brain finds this propagation delay, it can
	      determine the sound direction.  In an attempt to model
	      what the brain might do, RU signal processors want to
	      design an <emphasis>optimal</emphasis> system that
	      delays each ear's signal by some amount then adds them
	      together.	      
	      <m:math>
		<m:ci>
		  <m:msub>
		    <m:mi>Δ</m:mi>
		    <m:mi>l</m:mi>
		  </m:msub>
		</m:ci>
	      </m:math> 	      
	      and	      
	      <m:math>
		<m:ci>
		  <m:msub>
		    <m:mi>Δ</m:mi>
		    <m:mi>r</m:mi>
		  </m:msub>
		</m:ci>
	      </m:math>   
	      are the delays applied to the left and right signals
	      respectively.  The idea is to determine the delay values
	      according to some criterion that is based on what is
	      measured by the two ears.
	      
	      <list id="list4.8" type="enumerated">
		<item>
		  What is the transfer function between the sound signal
		  <m:math>
		    <m:apply>
		      <m:ci type="fn">s</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:math>
		  and the processor output 
		  <m:math>
		    <m:apply>
		      <m:ci type="fn">y</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:math>?
		</item>
		<item>
		  One way of determining the delay
		  <m:math><m:ci>τ</m:ci></m:math> is to choose
		  <m:math>
		    <m:ci>
		      <m:msub>
			<m:mi>Δ</m:mi>
			<m:mi>l</m:mi>
		      </m:msub>
		    </m:ci>
		  </m:math> 		  
		  and		  
		  <m:math>
		    <m:ci>
		      <m:msub>
			<m:mi>Δ</m:mi>
			<m:mi>r</m:mi>
		      </m:msub>
		    </m:ci>
		  </m:math>		  
		  to maximize the power in		  
		  <m:math>
		    <m:apply>
		      <m:ci type="fn">y</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:math>.  
		  How are these maximum-power processing delays
		  related to <m:math><m:ci>τ</m:ci></m:math>?
		</item>		
	      </list>
	    </para>
	  </section>
	</q:question>	
      </q:item>


      <q:item id="i9" type="text-response"> <!--problem 9 -->
        <q:question>
	  <section id="s9">
	    <name>Arrangements of Systems</name>
	    <para id="p9">
	      Architecting a system of modular components means
	      arranging them in various configurations to achieve some
	      overall input-output relation.  For each of the <cnxn target="fig4.9" strength="9">following</cnxn>, determine
	      the overall transfer function between
	      <m:math>
		<m:apply>
		  <m:ci type="fn">x</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>	      
	      and	      
	      <m:math display="inline">
		<m:apply>
		  <m:ci type="fn">y</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>.
	    </para>

	    <figure orient="vertical" id="fig4.9">
	      <subfigure>
		<name>system a</name>
		<media type="image/png" src="sys1.png"/>
	      </subfigure>
	      <subfigure>
		<name>system b</name>
		<media type="image/png" src="sys2.png"/>
	      </subfigure>
	      <subfigure>
		<name>system c</name>
		<media type="image/png" src="sys3.png"/>
	      </subfigure>
	    </figure>

	    <para id="lastquestion">
	      The overall transfer function for the cascade (first
	      depicted system) is particularly interesting.  What does
	      it say about the effect of the ordering of linear,
	      time-invariant systems in a cascade?
	    </para>	    
	  </section>
	</q:question>	
      </q:item>

      
      <q:item id="i9a" type="text-response"> <!--problem 9a -->
        <q:question>
	  <section id="s9a">
	    <name>Filtering</name>
	    <para id="p9a">
	      Let the signal
	      <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:divide/>
		        <m:apply><m:sin/>
		          <m:apply><m:times/>
		            <m:pi/>
		            <m:ci>t</m:ci>
		          </m:apply>
		        </m:apply>
		        <m:apply><m:times/>
		          <m:pi/>
		          <m:ci>t</m:ci>
		        </m:apply>
		      </m:apply>
		    </m:apply>
	      </m:math> be the input to a linear, time-invariant filter having the transfer function shown <cnxn target="fig4.9a">below</cnxn>.
	      Find the expression for
	      <m:math>
            <m:apply><m:ci type="fn">y</m:ci><m:ci>t</m:ci></m:apply>
	      </m:math>, the filter's output.
	    </para>
	    <figure orient="vertical" id="fig4.9a">
	      <media type="image/png" src="spectrum20.png"/>
	    </figure>
	  </section>
	</q:question>	
      </q:item>

      <q:item id="i9b" type="text-response"> <!--problem 9b -->
        <q:question>
	  <section id="s9b">
	    <name>Circuits Filter!</name>
	    <para id="p9b">
	    A unit-amplitude pulse with duration of one second serves as the input to an RC-circuit having transfer function
	    <m:math display="block">
	      <m:apply><m:eq/>
	        <m:apply><m:ci type="fn">H</m:ci><m:ci>f</m:ci></m:apply>
	        <m:apply><m:divide/>
	          <m:apply><m:times/>
	            <m:imaginaryi/><m:cn>2</m:cn><m:pi/><m:ci>f</m:ci>
	          </m:apply>
	          <m:apply><m:plus/>
	            <m:cn>4</m:cn>
	            <m:apply><m:times/>
	              <m:imaginaryi/><m:cn>2</m:cn><m:pi/><m:ci>f</m:ci>
	            </m:apply>
	          </m:apply>
	        </m:apply>
	      </m:apply>
	    </m:math>
	    
	    <list id="parts9b" type="enumerated">
	      <item>
	        How would you categorize this transfer function:
	        lowpass, highpass, bandpass, other?
	      </item>
	      <item>
	        Find a circuit that corresponds to this transfer function.
	      </item>
	      <item>
	        Find an expression for the filter's output.
	      </item>
	    </list>
	    </para>

	  </section>
	  </q:question>	
      </q:item>


      <q:item id="i10" type="text-response"> <!--problem 10 -->
        <q:question>
	  <section id="s10">
	    <name>Reverberation</name>
	    <para id="p10">
	      Reverberation corresponds to adding to a signal its
	      delayed version.
	      
	      <list id="list4.10" type="enumerated">
		<item>
		  Assuming <m:math><m:ci>τ</m:ci></m:math>
		  represents the delay, what is the input-output
		  relation for a reverberation system?  Is the system
		  linear and time-invariant?  If so, find the transfer
		  function; if not, what linearity or time-invariance
		  criterion does reverberation violate.  </item>
		<item>
		  A music group known as the ROwls is having trouble
		  selling its recordings.  The record company's
		  engineer gets the idea of applying different delay
		  to the low and high frequencies and adding the
		  result to create a new musical effect.  Thus, the
		  ROwls' audio would be separated into two parts (one
		  less than the frequency		  
		  <m:math>
		    <m:ci>
		      <m:msub>
			<m:mi>f</m:mi>
			<m:mn>0</m:mn>
		      </m:msub>
		    </m:ci>
		  </m:math>, 
		  the other greater than 
		  <m:math>
		    <m:ci>
		      <m:msub>
			<m:mi>f</m:mi>
			<m:mn>0</m:mn>
		      </m:msub>
		    </m:ci>
		  </m:math>), 
		  these would be delayed by		  
		  <m:math>
		    <m:ci>
		      <m:msub>
			<m:mi>τ</m:mi>
			<m:mi>l</m:mi>
		      </m:msub>
		    </m:ci>
		  </m:math>		  
		  and		  
		  <m:math>
		    <m:ci>
		      <m:msub>
			<m:mi>τ</m:mi>
			<m:mi>h</m:mi>
		      </m:msub>
		    </m:ci>
		  </m:math>  
		  respectively, and the resulting signals added.  Draw
		  a block diagram for this new audio processing
		  system, showing its various components.
		</item>

		<item>
		  How does the magnitude of the system's transfer
		  function depend on the two delays?
		</item>		
	      </list>
	    </para>
	  </section>
	</q:question>	
      </q:item>


      <q:item id="i11" type="text-response"> <!--problem 11 -->
        <q:question>
	  <section id="sec11">
	    <name>Echoes in Telephone Systems</name>
	    <para id="p11">
	      A frequently encountered problem in telephones is echo.
	      Here, because of acoustic coupling between the ear piece
	      and microphone in the handset, what you hear is also
	      sent to the person talking.  That person thus not only
	      hears you, but also hears her own speech delayed
	      (because of propagation delay over the telephone
	      network) and attenuated (the acoustic coupling gain is
	      less than one).  Furthermore, the same problem applies
	      to you as well: The acoustic coupling occurs in her
	      handset as well as yours.

	      <list id="list4.11" type="enumerated">
		<item>
		  Develop a block diagram that describes this
		  situation.
		</item>
		<item>
		  Find the transfer function between your voice and
		  what the listener hears.
		</item>
		<item>
		  Each telephone contains a system for reducing echoes
		  using electrical means.  What simple system could
		  null the echoes?
		</item>		
	      </list>
	    </para>
	  </section>
	</q:question>	
      </q:item>


      <q:item id="i12" type="text-response"> <!--problem 12 -->
        <q:question>
	  <section id="s12">
	    <name>Demodulating an AM Signal</name>
	    <para id="p12">
	      Let 
	      <m:math>
		<m:apply>
		  <m:ci type="fn">m</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>	      
	      denote the signal that has been amplitude modulated.
	      
	      <m:math display="block">
		<m:apply>
		  <m:eq/>
		  <m:apply>
		    <m:ci type="fn">x</m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:times/>
		    <m:ci>A</m:ci>
		    <m:apply>
		      <m:plus/>
		      <m:cn>1</m:cn>
		      <m:apply>   
			<m:ci type="fn">m</m:ci>
			<m:ci>t</m:ci>
		      </m:apply>
		    </m:apply>
		    <m:apply>
		      <m:sin/>
		      <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:math>
	      
	      Radio stations try to restrict the amplitude of the
	      signal
	      <m:math>
		<m:apply>
		  <m:ci type="fn">m</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>
	      so that it is less than one in magnitude.  The frequency
	      <m:math>
		<m:ci>
		  <m:msub>
		    <m:mi>f</m:mi>
		    <m:mi>c</m:mi>
		  </m:msub>
		</m:ci> 
	      </m:math>
	      is very large compared to the frequency content of the
	      signal.  What we are concerned about here is not
	      transmission, but reception.
	      
	      <list id="list4.12" type="enumerated">
		<item>
		  The so-called coherent demodulator simply multiplies
		  the signal		  
		  <m:math>
		    <m:apply>
		      <m:ci type="fn">x</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:math>		  
		  by a sinusoid having the same frequency as the
		  carrier and lowpass filters the result.  Analyze
		  this receiver and show that it works.  Assume the
		  lowpass filter is ideal.
		</item>		
		<item>
		  One issue in coherent reception is the phase of the
		  sinusoid used by the receiver relative to that used
		  by the transmitter.  Assuming that the sinusoid of
		  the receiver has a phase
		  <m:math><m:ci>φ</m:ci></m:math>, how does the
		  output depend on
		  <m:math><m:ci>φ</m:ci></m:math>?  What is the
		  worst possible value for this phase?
		</item>
		<item>
		  The incoherent receiver is more commonly used
		  because of the phase sensitivity problem inherent in
		  coherent reception.  Here, the receiver full-wave
		  rectifies the received signal and lowpass filters
		  the result (again ideally).  Analyze this receiver.
		  Does its output differ from that of the coherent
		  receiver in a significant way?
		</item>		
	      </list>
	    </para>
	  </section>
	</q:question>	
      </q:item>

      <q:item id="i12a" type="text-response"> <!--problem 12a -->
        <q:question>
	  <section id="s12a">
	    <name>Unusual Amplitude Modulation</name>
	    <para id="p12a">
	    We want to send a band-limited signal having the
	    <cnxn target="fig12aa">depicted spectrum</cnxn> with amplitude modulation in the usual way.
	    I.B. Different suggests using the square-wave carrier shown <cnxn target="fig12ab">below</cnxn>.
	    Well, it is different, but his friends wonder if any technique can demodulate it.
	    <list id="parts12a" type="enumerated">
	      <item>
	        Find an expression for
	        <m:math>
	          <m:apply><m:ci type="fn">X</m:ci><m:ci>f</m:ci></m:apply>
	        </m:math>, the Fourier transform of the modulated signal.
	      </item>
	      <item>
	        Sketch the magnitude of
	        <m:math>
	          <m:apply><m:ci type="fn">X</m:ci><m:ci>f</m:ci></m:apply>
	        </m:math>, being careful to label important magnitudes and frequencies.
	      </item>
	      <item>
	        What demodulation technique obviously works?
	      </item>
	      <item>
	        I.B. challenges three of his friends to demodulate
	        <m:math>
	          <m:apply><m:ci type="fn">x</m:ci><m:ci>t</m:ci></m:apply>
	        </m:math> some other way.
	        One friend suggests modulating 
	        <m:math>
	          <m:apply><m:ci type="fn">x</m:ci><m:ci>t</m:ci></m:apply>
	        </m:math> with
	        <m:math>
	          <m:apply><m:cos/>
	            <m:apply><m:divide/>
	              <m:apply><m:times/>
	                <m:pi/> <m:ci>t</m:ci>
	              </m:apply>
	              <m:cn>2</m:cn>
	            </m:apply>
	          </m:apply>
	        </m:math>, another wants to try modulating with
	        <m:math>
	          <m:apply><m:cos/>
	            <m:apply><m:times/>
	              <m:pi/> <m:ci>t</m:ci>
	            </m:apply>
	          </m:apply>
	        </m:math> and the third thinks
	        <m:math>
	          <m:apply><m:cos/>
	            <m:apply><m:divide/>
	              <m:apply><m:times/>
	                <m:cn>3</m:cn> <m:pi/> <m:ci>t</m:ci>
	              </m:apply>
	              <m:cn>2</m:cn>
	            </m:apply>
	          </m:apply>
	        </m:math> will work.
	        Sketch the magnitude of the Fourier transform of the signal each student's approach produces.
	        Which student comes closest to recovering the original signal?
	        Why?
	      </item>
	    </list>
	    <figure orient="vertical" id="fig12a">
	      <subfigure id="fig12aa">
	        <media type="image/png" src="spectrum21a.png"/>
	      </subfigure>
	      <subfigure id="fig12ab">
	        <media type="image/png" src="spectrum21b.png"/>
	      </subfigure>
	    </figure>
	    </para>

	  </section>
	  </q:question>	
      </q:item>

      
      <q:item id="iq2.3" type="text-response"> <!--problem 13 -->
        <q:question>
	  <section id="sq2.3">
	    <name>Sammy Falls Asleep...</name>
	    <para id="pq2.3">
	      While sitting in ELEC 241 class, he falls asleep during
	      a critical time when an AM receiver is being described.
	      The received signal has the form	      
	      <m:math>
		<m:apply>
		  <m:eq/>
		  <m:apply>
		    <m:ci type="fn">r</m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:times/>
		    <m:ci>A</m:ci>
		    <m:apply>
		      <m:plus/>
		      <m:cn>1</m:cn>
		      <m:apply>
			<m:ci type="fn">m</m:ci>
			<m:ci>t</m:ci>
		      </m:apply>
		    </m:apply>
		    <m:apply>
		      <m:cos/>
		      <m:apply>
			<m:plus/>
			<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:ci>φ</m:ci>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:math>	      
	      where the phase 
	      <m:math>
		<m:ci>φ</m:ci>
	      </m:math>
	      is unknown. The message signal is
	      <m:math>
		<m:apply>
		  <m:ci type="fn">m</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>;
	      it has a bandwidth of 
	      <m:math><m:ci>W</m:ci></m:math> Hz 
	      and a magnitude less than 1 
	      (<m:math>
		<m:apply>
		  <m:lt/>
		  <m:apply>
		    <m:abs/>
		    <m:apply>
		      <m:ci type="fn">m</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		  <m:cn>1</m:cn>
		</m:apply>
	      </m:math>).
	      The phase 
	      <m:math>
		<m:ci>φ</m:ci>
	      </m:math>
	      is unknown. The instructor drew a <cnxn target="sys34" strength="9">diagram</cnxn> for a receiver on the board;
	      Sammy slept through the description of what the unknown
	      systems where.
	    </para>
	    
	    <figure id="sys34">
	      <media type="image/png" src="sys34.png"/>
	    </figure>

	    <para id="pq2.3_2">
	      <list id="lq2.3" type="enumerated">
		<item>
		  What are the signals
		  <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>
		  and
		  <m:math>
		    <m:apply>
		      <m:ci type="fn">
			<m:msub>
			  <m:mi>x</m:mi>
			  <m:mi>s</m:mi>
			</m:msub>
		      </m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:math>?
		</item>
		<item>
		  What would you put in for the unknown systems that
		  would guarantee that the final output contained the
		  message regardless of the phase?

		  <note type="hint">
		    Think of a trigonometric identity that would prove
		    useful. 
		  </note>
		</item>

		<item>
		  Sammy may have been asleep, but he can think of a far
		  simpler receiver.  What is it?
		</item>
	      </list>
	    </para>
	  </section>
	</q:question>
      </q:item>

      
      <q:item id="i13" type="text-response"> <!--problem 14 -->
        <q:question>
	  <section id="s13">
	    <name>Jamming</name>
	    <para id="p13">
	      Sid Richardson college decides to set up its own AM
	      radio station KSRR.  The resident electrical engineer
	      decides that she can choose <emphasis>any</emphasis>
	      carrier frequency and message bandwidth for the station.
	      A rival college decides to <term>jam</term> its
	      transmissions by transmitting a high-power signal that
	      interferes with radios that try to receive KSRR.  The
	      jamming signal
	      <m:math>
		<m:apply>
		  <m:ci type="fn">jam</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>
	      is what is known as a <term>sawtooth</term> <cnxn target="fig4.13" strength="9"/> wave having a period
	      known to KSRR's engineer.
	    </para>
	    
	    <figure id="fig4.13">
	      <media type="image/png" src="sig41.png"/>
	    </figure>
	    
	    <list id="list4.13" type="enumerated">
	      <item>
		Find the spectrum of the jamming signal.
	      </item>
	      <item>
		Can KSRR entirely circumvent the attempt to jam it by
		carefully choosing its carrier frequency and
		transmission bandwidth?  If so, find the station's
		carrier frequency and transmission bandwidth in terms
		of 
		<m:math>
		  <m:ci>T</m:ci>
		</m:math>,
		the period of the jamming signal; if not, show
		why not.
	      </item>	      
	    </list>
	  </section>
	</q:question>	
      </q:item>
      
      
      <q:item id="i14" type="text-response"> <!-- problem 16  -->
        <q:question>
	  <section id="s14">
	    <name>AM Stereo</name>
	    <para id="p14">
	      A stereophonic signal consists of a "left" signal	      
	      <m:math display="inline">
		<m:apply>
		  <m:ci type="fn">l</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>	      
	      and a "right" signal	      
	      <m:math display="inline">
		<m:apply>
		  <m:ci type="fn">r</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>	      
	      that conveys sounds coming from an orchestra's left and
	      right sides, respectively.  To transmit these two
	      signals simultaneously, the transmitter first forms the
	      sum signal	      
	      <m:math display="inline">
		<m:apply>
		  <m:eq/>
		  <m:apply>
		    <m:ci type="fn">
		      <m:msub>
			<m:mi>s</m:mi>
			<m:mo>+</m:mo>
		      </m:msub>
		    </m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:plus/>
		    <m:apply>
		      <m:ci type="fn">l</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		    <m:apply>
		      <m:ci type="fn">r</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:math>	      
	      and the difference signal	      
	      <m:math>
		<m:apply>
		  <m:eq/>
		  <m:apply>
		    <m:ci type="fn">
		      <m:msub>
			<m:mi>s</m:mi>
			<m:mo>-</m:mo>
		      </m:msub>
		    </m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:minus/>
		    <m:apply>
		      <m:ci type="fn">l</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		    <m:apply>
		      <m:ci type="fn">r</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:math>.
	      Then, the transmitter amplitude-modulates the difference
	      signal with a sinusoid having frequency
	      <m:math>
		<m:apply>
		  <m:times/>
		  <m:cn>2</m:cn>
		  <m:ci>W</m:ci>
		</m:apply>
	      </m:math>, 
	      where 
	      <m:math>
		<m:ci>W</m:ci>
	      </m:math>
	      is the bandwidth of the left and right signals.  The sum
	      signal and the modulated difference signal are added,
	      the sum amplitude-modulated to the radio station's
	      carrier frequency
	      <m:math display="inline">
		<m:ci type="fn">
		  <m:msub>
		    <m:mi>f</m:mi>
		    <m:mi>c</m:mi>
		  </m:msub>
		</m:ci>
	      </m:math>, and transmitted.  Assume the spectra of the
	      left and right signals are <cnxn target="fig4.14" strength="9">as shown</cnxn>.
	    </para>
	    
	    <figure id="fig4.14">
	      <media type="image/png" src="spectrum13.png"/>
	    </figure>
	    
	    <list id="list4.14" type="enumerated">
	      <item>
		What is the expression for the transmitted signal?
		Sketch its spectrum.
	      </item>
	      <item>
		Show the block diagram of a stereo AM receiver that
		can yield the left and right signals as separate
		outputs.
	      </item>
	      <item>		
		What signal would be produced by a conventional
		coherent AM receiver that expects to receive a
		standard AM signal conveying a message signal having
		bandwidth
		<m:math>
		  <m:ci>W</m:ci>
		</m:math>?
	      </item>	      
	    </list>
	  </section>
	</q:question>	
      </q:item>


      <q:item id="i15" type="text-response"> <!-- problem 17 -->
        <q:question>
	  <section id="s15">
	    <name>Novel AM Stereo Method</name>
	    <para id="p15">
	      A clever engineer has submitted a patent for a new
	      method for transmitting two signals
	      <emphasis>simultaneously</emphasis> in the
	      <emphasis>same</emphasis> transmission bandwidth as
	      commercial AM radio.  <cnxn target="fig4.15" strength="9">As shown</cnxn>, her approach is to
	      modulate the positive portion of the carrier with one
	      signal and the negative portion with a second.    
	    <figure id="fig4.15">
	      <media type="image/png" src="amstereo.png"/>
	    </figure>
	      In detail the two message signals	      
	      <m:math>
		<m:apply>
		  <m:ci type="fn">
		    <m:msub>
		      <m:mi>m</m:mi>
		      <m:mn>1</m:mn>
		    </m:msub>
		  </m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>	      
	      and	      
	      <m:math>
		<m:apply>
		  <m:ci type="fn">
		    <m:msub>
		      <m:mi>m</m:mi>
		      <m:mn>2</m:mn>
		    </m:msub>
		  </m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>	      
	      are bandlimited to 
	      <m:math>
		<m:ci>W</m:ci>
	      </m:math>
	      Hz and have maximal amplitudes equal to 1.  The carrier
	      has a frequency	      
	      <m:math>
		<m:ci>
		  <m:msub>
		    <m:mi>f</m:mi>
		    <m:mi>c</m:mi>
		  </m:msub>
		</m:ci>
	      </m:math>	      
	      much greater than 
	      <m:math>
		<m:ci>W</m:ci>
	      </m:math>.
	      The transmitted signal	      
	      <m:math>
		<m:apply>
		  <m:ci type="fn">x</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>	      
	      is given by
	      
	      <m:math display="block">
		<m:apply>
		  <m:eq/>
		  <m:apply>
		    <m:ci type="fn">x</m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:piecewise>
		    <m:piece>
		      <m:apply>
			<m:times/>
			<m:ci>A</m:ci>
			<m:apply>
			  <m:plus/>
			  <m:cn>1</m:cn>
			  <m:apply> 
			    <m:times/>
			    <m:ci>a</m:ci>
			    <m:apply>  
			      <m:ci type="fn">
				<m:msub>
				  <m:mi>m</m:mi>
				  <m:mn>1</m:mn>
				</m:msub>
			      </m:ci>
			      <m:ci>t</m:ci>
			    </m:apply>
			  </m:apply>
			</m:apply>
			<m:apply>
			  <m:sin/>
			  <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:geq/>
			<m:apply>
			  <m:sin/>
			  <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:cn>0</m:cn>
		      </m:apply>
		    </m:piece>
		    <m:piece>
		      <m:apply>
			<m:times/>
			<m:ci>A</m:ci>
			<m:apply>
			  <m:plus/>
			  <m:cn>1</m:cn>
			  <m:apply> 
			    <m:times/>
			    <m:ci>a</m:ci>
			    <m:apply>  
			      <m:ci type="fn">
				<m:msub>
				  <m:mi>m</m:mi>
				  <m:mn>2</m:mn>
				</m:msub>
			      </m:ci>
			      <m:ci>t</m:ci>
			    </m:apply>
			  </m:apply>
			</m:apply>
			<m:apply>
			  <m:sin/>
			  <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:lt/>
			<m:apply>
			  <m:sin/>
			  <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:cn>0</m:cn>
		      </m:apply>
		    </m:piece>     
		  </m:piecewise>
		</m:apply>
	      </m:math>
	      
	      In all cases, 
	      <m:math>
		<m:apply>
		  <m:lt/>
		  <m:cn>0</m:cn>
		  <m:ci>a</m:ci>
		  <m:cn>1</m:cn>
		</m:apply>
	      </m:math>.  
	      The plot shows the transmitted signal when the messages
	      are sinusoids:
	      <m:math>
		<m:apply>
		  <m:eq/>
		  <m:apply>
		    <m:ci type="fn">
		      <m:msub>
			<m:mi>m</m:mi>
			<m:mn>1</m:mn>
		      </m:msub>
		    </m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:sin/>
		    <m:apply>
		      <m:times/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		      <m:ci>
			<m:msub>
			  <m:mi>f</m:mi>
			  <m:mi>m</m:mi>
			</m:msub>
		      </m:ci> 
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:math> 	      
	      and
	      <m:math>
		<m:apply>
		  <m:eq/>
		  <m:apply>
		    <m:ci type="fn">
		      <m:msub>
			<m:mi>m</m:mi>
			<m:mn>2</m:mn>
		      </m:msub>
		    </m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:sin/>
		    <m:apply>
		      <m:times/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		      <m:cn>2</m:cn>
		      <m:ci>
			<m:msub>
			  <m:mi>f</m:mi>
			  <m:mi>m</m:mi>
			</m:msub>
		      </m:ci> 
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:math> 	      
	      where	      
	      <m:math>
		<m:apply>
		  <m:lt/>
		  <m:apply>
		    <m:times/>
		    <m:cn>2</m:cn>
		    <m:ci>
		      <m:msub>
			<m:mi>f</m:mi>
			<m:mi>m</m:mi>
		      </m:msub>
		    </m:ci>
		  </m:apply>
		  <m:ci>W</m:ci>
		</m:apply>
	      </m:math>.
	      You, as the patent examiner, must determine whether the
	      scheme meets its claims and is useful.

	      <list id="list4.15" type="enumerated">
		<item>
                  Provide a more concise expression for the
                  transmitted signal <m:math><m:apply><m:ci type="fn">x</m:ci><m:ci>t</m:ci></m:apply></m:math>
                  than given above.
                </item>

                <item>
		  What is the receiver for this scheme? It would yield
		  both 		  
		  <m:math>
		    <m:apply>
		      <m:ci type="fn">
			<m:msub>
			  <m:mi>m</m:mi>
			  <m:mn>1</m:mn>
			</m:msub>
		      </m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:math>		  
		  and 		  
		  <m:math>
		    <m:apply>
		      <m:ci type="fn">
			<m:msub>
			  <m:mi>m</m:mi>
			  <m:mn>2</m:mn>
			</m:msub>
		      </m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:math>		  
		  from		  
		  <m:math>
		    <m:apply>
		      <m:ci type="fn">x</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:math>.
		</item>		
		<item>
		  Find the spectrum of the positive portion of the
		  transmitted signal.
		</item>
		<item>
		  Determine whether this scheme satisfies the design
		  criteria, allowing you to grant the patent.  Explain
		  your reasoning.
		</item>		
	      </list>
	    </para>
	  </section>
	</q:question>	
      </q:item>

      
      <q:item id="i16" type="text-response"> <!-- problem 18 -->
        <q:question>
	  <section id="s16">
	    <name>A Radical Radio Idea</name>
	    <para id="p16">
	      An ELEC 241 student has the bright idea of using a
	      square wave instead of a sinusoid as an AM carrier. The
	      transmitted signal would have the form
	      
	      <m:math display="block">
		<m:apply>
		  <m:eq/>
		  <m:apply>
		    <m:ci type="fn">x</m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:times/>
		    <m:ci>A</m:ci>
		    <m:apply>
		      <m:plus/>
		      <m:cn>1</m:cn>
		      <m:apply>   
			<m:ci type="fn">m</m:ci>
			<m:ci>t</m:ci>
		      </m:apply>
		    </m:apply>
		    <m:apply>
		      <m:ci type="fn">
			<m:msub>
			  <m:mi>sq</m:mi>
			  <m:mi>T</m:mi>
			</m:msub>
		      </m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:math> 
	      
	      where the message signal 	      
	      <m:math>
		<m:apply>
		  <m:ci type="fn">m</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math>	      
	      would be amplitude-limited:	      
	      <m:math>
		<m:apply>
		  <m:lt/>
		  <m:apply>
		    <m:abs/>    
		    <m:apply>  
		      <m:ci type="fn">m</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		  <m:cn>1</m:cn>
		</m:apply>
	      </m:math>
	      
	      <list id="list4.16" type="enumerated">
		<item>
		  Assuming the message signal is lowpass and has a
		  bandwidth of
		  <m:math>
		    <m:ci>W</m:ci>
		  </m:math> Hz,
		  what values for the square wave's period
		  <m:math>
		    <m:ci>T</m:ci>
		  </m:math>		  
		  are feasible.  In other words, do some combinations
		  of
		  <m:math>
		    <m:ci>W</m:ci>
		  </m:math> 
		  and
		  <m:math>
		    <m:ci>T</m:ci>
		  </m:math>
		  prevent reception?
		</item> 
		<item>
		  Assuming reception is possible, can
		  <emphasis>standard</emphasis> radios receive this
		  innovative AM transmission?  If so, show how a
		  coherent receiver could demodulate it; if not, show
		  how the coherent receiver's output would be
		  corrupted.  Assume that the message bandwidth
		  <m:math>
		    <m:apply>
		      <m:eq/>
		      <m:ci>W</m:ci>
		      <m:apply>
			<m:times/>		      
			<m:cn>5</m:cn>
			<m:ci>kHz</m:ci>
		      </m:apply>
		    </m:apply> 
		  </m:math>.
		</item>
	      </list>
	    </para>
	  </section>
	</q:question>	
      </q:item>

      <q:item id="iq2.3a" type="text-response">
        <q:question>
	  <section id="sq2.3a">
	    <name>Secret Communication</name>
	    <para id="pq2.3a">An amplitude-modulated secret message
	      <m:math>
		<m:apply>
		  <m:ci type="fn">m</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math> has the following form.
	      <m:math display="block">
		<m:apply>
		  <m:eq/>
		  <m:apply>
		    <m:ci type="fn">r</m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:times/>
		    <m:ci>A</m:ci>
		    <m:apply>
		      <m:plus/>
		      <m:cn>1</m:cn>
		      <m:apply>
			<m:ci type="fn">m</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:apply>
			  <m:plus/>
			  <m:ci><m:msub>
			      <m:mi>f</m:mi>
			      <m:mi>c</m:mi>
			    </m:msub></m:ci>
			  <m:ci><m:msub>
			      <m:mi>f</m:mi>
			      <m:mn>0</m:mn>
			    </m:msub></m:ci>
			</m:apply>
			<m:ci>t</m:ci>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:math>
	      The message signal has a bandwidth of
	      <m:math>
		  <m:ci>W</m:ci>
	      </m:math> Hz and a magnitude less than 1
	      (<m:math>
		<m:apply>
		  <m:lt/>
		  <m:apply>
		    <m:abs/>
		    <m:apply>
		      <m:ci type="fn">m</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		  <m:cn>1</m:cn>
		</m:apply>
	      </m:math>). The idea is to offset the carrier frequency by
	      <m:math>
		  <m:ci><m:msub>
		      <m:mi>f</m:mi>
		      <m:mn>0</m:mn>
		    </m:msub></m:ci>
	      </m:math> Hz
	      from standard radio carrier frequencies. Thus,
	      "off-the-shelf" coherent demodulators would assume the
	      carrier frequency has
	      <m:math>
		  <m:ci><m:msub>
		      <m:mi>f</m:mi>
		      <m:mi>c</m:mi>
		    </m:msub></m:ci>
	      </m:math> Hz. Here, 
	      <m:math>
		<m:apply>
		  <m:lt/>
		  <m:ci><m:msub>
		      <m:mi>f</m:mi>
		      <m:mn>0</m:mn>
		    </m:msub></m:ci>
		  <m:ci>W</m:ci>
		</m:apply>
	      </m:math>.
	    </para>

	    <list id="lq2.3a" type="enumerated">
	      <item>Sketch the spectrum of the demodulated signal
	      produced by a coherent demodulator tuned to
		<m:math>
		    <m:ci><m:msub>
			<m:mi>f</m:mi>
			<m:mi>c</m:mi>
		      </m:msub></m:ci>
		</m:math> Hz.
	      </item>

	      <item>Will this demodulated signal be a “scrambled”
	      version of the original? If so, how so; if not, why not?
	      </item>

	      <item>Can you develop a receiver that can demodulate the
	      message without knowing the offset frequency
		<m:math>
		  <m:ci><m:msub>
		      <m:mi>f</m:mi>
		      <m:mi>c</m:mi>
		    </m:msub></m:ci>
		</m:math>?
	      </item>
	    </list>
	  </section>
	</q:question>
      </q:item>

      <q:item id="iF2" type="text-response"> 
        <q:question>
	  <section id="sF2">
	    <name>Signal Scrambling</name> 

	    <para id="pF2">An excited inventor announces the discovery
	    of a way of using analog technology to render music
	    unlistenable without knowing the secret recovery
	    method. The idea is to modulate the bandlimited message
	      <m:math>
		<m:apply>
		  <m:ci type="fn">m</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math> by a special periodic signal
	      <m:math>
		<m:apply>
		  <m:ci type="fn">s</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:math> that is zero during half of its period, which
	      renders the message unlistenable and superficially, at
	      least, unrecoverable (<cnxn target="figF2" strength="9"/>).
	    </para>

	    <figure id="figF2">
	      <media type="image/png" src="sig49.png"/>
	    </figure>
	    
	    <list id="lF2" type="enumerated">
	      <item>What is the Fourier series for the periodic
	      signal?</item>
	      
	      <item>What are the restrictions on the period
	      <m:math><m:ci>T</m:ci></m:math> so that the message
	      signal can be recovered from
		<m:math>
		  <m:apply>
		    <m:times/>
		    <m:apply>
		      <m:ci type="fn">m</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		    <m:apply>
		      <m:ci type="fn">s</m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		</m:math>?
	      </item>

	      <item>ELEC 241 students think they have "broken" the
	      inventor's scheme and are going to announce it to the
	      world. How would they recover the original message
	      <emphasis>without</emphasis> having detailed knowledge
	      of the modulating signal?
	      </item>
	    </list>
	  </section>
	</q:question>
      </q:item>

    </q:problemset>
  </content>
</document>
