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  <name xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Dirichlet Conditions</name>
  
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      <md:surname xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Haag</md:surname>
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  <md:keywordlist xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
    <md:keyword xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">dirichlet conditions</md:keyword>
    <md:keyword xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">fourier</md:keyword>
    <md:keyword xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">fourier series</md:keyword>
    <md:keyword xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">fourier transform</md:keyword>
    <md:keyword xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">strong dirichlet condition</md:keyword>
    <md:keyword xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">weak dirichlet condition</md:keyword>
  </md:keywordlist>

  <md:abstract xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">The Dirichlet conditions are the sufficient conditions to guarantee existence and convergence of the Fourier series or the Fourier transform.

</md:abstract>
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  <content xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
    <para 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="p1">
      Named after the German mathematician, Peter Dirichlet, the
      <term xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Dirichlet conditions</term> are the sufficient conditions
      to guarantee <term xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">existence</term> and <term xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">convergence</term>
      of the <cnxn xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" document="m10496" strength="8">Fourier series</cnxn>
      or the <cnxn xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" document="m0046" strength="8">Fourier
      transform</cnxn>.
    </para>
    
    <section 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="sec1">
      <name xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">The Weak Dirichlet Condition for the Fourier Series</name>
      <rule xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" type="condition" id="rule1">
	<name xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">The Weak Dirichlet Condition</name>
	<statement xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
	  <para 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="p2">
	    For the Fourier Series to exist, the Fourier coefficients
	    must be finite.  The <term xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Weak Dirichlet Condition</term>
	    guarantees this existence.  It essentially says that the
	    integral of the absolute value of the signal must be
	    finite.  The limits of integration are different for the
	    Fourier Series case than for the Fourier Transform case.
	    This is a direct result of the differing definitions of
	    the two.
	  </para>
	</statement>

	<proof xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
	  <para 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="p3">
	    The Fourier Series exists (the coefficients are finite) if

	    <equation 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="eqn1">
	      <name xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
		Weak Dirichlet Condition for the Fourier Series
	      </name>
	      <m:math>
		<m:apply>
		  <m:lt/>
		  <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:abs/>
		      <m:apply>
			<m:ci type="fn">f</m:ci>
			<m:ci>t</m:ci>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		  <m:infinity/>
		</m:apply>
	      </m:math>
	    </equation>

	    This can be shown from the initial condition that the Fourier
	    Series coefficients be finite.

	    <equation 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="eqn2">
	      <m:math display="display">
		<m:apply>
		  <m:leq/>
		  <m:apply>
		    <m:eq/>
		    <m:apply>
		      <m:abs/>
		      <m:apply>
			<m:ci>
			  <m:msub>
			    <m:mi>c</m:mi>
			    <m:mi>n</m:mi>
			  </m:msub>
			</m:ci>
		      </m:apply>
		    </m:apply>
		    <m:apply>
		      <m:abs/>
		      <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:times/>
			    <m:apply>
			      <m:ci type="fn">f</m:ci>
			      <m:ci>t</m:ci>
			    </m:apply>
			    <m:apply>
			      <m:exp/>
			      <m:apply>
				<m:minus/>
				<m:apply>
				  <m:times/>
				  <m:imaginaryi/>
				  <m:apply>
				    <m:ci>
				      <m:msub>
					<m:mi>ω</m:mi>
					<m:mn>0</m:mn>
				      </m:msub>
				    </m:ci>
				  </m:apply>
				  <m:ci>n</m:ci>
				  <m:ci>t</m:ci>
				</m:apply>
			      </m:apply>
			    </m:apply>
			  </m:apply>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </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:times/>
			<m:apply>
			  <m:abs/>
			  <m:apply>
			    <m:ci type="fn">f</m:ci>
			    <m:ci>t</m:ci>
			  </m:apply>
			</m:apply>
			<m:apply>
			  <m:abs/>
			  <m:apply>
			    <m:exp/>
			    <m:apply>
			      <m:minus/>
			      <m:apply>
				<m:times/>
				<m:imaginaryi/>
				<m:apply>
				  <m:ci>
				    <m:msub>
				      <m:mi>ω</m:mi>
				      <m:mn>0</m:mn>
				    </m:msub>
				  </m:ci>
				</m:apply>
				<m:ci>n</m:ci>
				<m:ci>t</m:ci>
			      </m:apply>
			    </m:apply>
			  </m:apply>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:math>
	    </equation>

	    Remembering our <cnxn xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" document="m10060" strength="7">complex
	    exponentials</cnxn>, we know that in the above equation
	    <m:math display="inline">
	      <m:apply>
		<m:eq/>
		<m:apply>
		  <m:abs/>
		  <m:apply>
		    <m:exp/>
		    <m:apply>
		      <m:minus/>
		      <m:apply>
			<m:times/>
			<m:imaginaryi/>
			<m:apply>
			  <m:ci>
			    <m:msub>
			      <m:mi>ω</m:mi>
			      <m:mn>0</m:mn>
			    </m:msub>
			  </m:ci>
			</m:apply>
			<m:ci>n</m:ci>
			<m:ci>t</m:ci>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
		<m:cn>1</m:cn>
	      </m:apply>
	    </m:math>, which gives us
	    
	    <equation 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="eqn4">
	      <m:math display="display">
		<m:apply>
		  <m:eq/>
		  <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:abs/>
			<m:apply>
			  <m:ci type="fn">f</m:ci>
			  <m:ci>t</m:ci>
			</m:apply>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:math>
	    </equation>

	    <equation 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="eqn5">
	      <m:math display="display">
		<m:apply>
		  <m:lt/>
		  <m:infinity/>
		</m:apply>
	      </m:math>
	    </equation>
	  </para>
	</proof>
      </rule>

      <para 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="sec2_p1">
	<note xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" type="note">
	  If we have the function:
	  
	  <m:math display="block">
	    <m:apply>
	      <m:forall/>
	      <m:bvar>
		<m:ci>t</m:ci>
	      </m:bvar>
	      <m:condition>
		<m:apply>
		  <m:leq/>
		  <m:apply>
		    <m:lt/>
		    <m:cn>0</m:cn>
		    <m:ci>t</m:ci>
		  </m:apply>
		  <m:ci>T</m:ci>
		</m:apply>
	      </m:condition>
	      <m:apply>
		<m:eq/>
		<m:apply>
		  <m:ci type="fn">f</m:ci>
		  <m:ci>t</m:ci>
		</m:apply>
		<m:apply>
		  <m:divide/>
		  <m:cn>1</m:cn>
		  <m:ci>t</m:ci>
		</m:apply>
	      </m:apply>
	    </m:apply>
	  </m:math>

	  then you should note that this functions
	  <emphasis xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">fails</emphasis> the above condition.
	</note>
      </para>
   
      <section 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="sec2">
	<name xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">The Weak Dirichlet Condition for the Fourier Transform</name>
	<rule xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" type="condition" id="rule2">
	  <statement xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
	    <para 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="p4">
	      The Fourier Transform exists if
	      <equation 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="eqn6">
		<name xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Weak Dirichlet Condition for the Fourier Transform</name>
		<m:math display="display">
		  <m:apply>
		    <m:lt/>
		    <m:apply>
		      <m:int/>
		      <m:bvar>
			<m:ci>t</m:ci>
		      </m:bvar>
		      <m:lowlimit>
			<m:apply>
			  <m:minus/>
			  <m:infinity/>
			</m:apply>
		      </m:lowlimit>
		      <m:uplimit>
			<m:infinity/>
		      </m:uplimit>
		      <m:apply>
			<m:abs/>
			<m:apply>
			  <m:ci type="fn">f</m:ci>
			  <m:ci>t</m:ci>
			</m:apply>
		      </m:apply>
		    </m:apply>
		    <m:infinity/>
		  </m:apply>
		</m:math>
	      </equation>

	      This can be derived the same way the weak Dirichlet for the
	      Fourier Series was derived, by beginning with the definition
	      and showing that the Fourier Transform must be less than
	      infinity everywhere.
	    </para>
	  </statement>
	</rule>
      </section>
    </section>

    <section 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="sec3">
      <name xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">The Strong Dirichlet Conditions</name>
      <para 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="p5">
	The Fourier Transform exists if the signal has a finite number
	of discontinuities and a finite number of <term xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">maxima</term>
	and <term xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">minima</term>.  For the Fourier Series to exist, the
	following two conditions must be satisfied (along with the Weak
	Dirichlet Condition):

	<list 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="list1" type="enumerated">
	  <item xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
	    In one period, 
	    <m:math>
	      <m:apply>
		<m:ci type="fn">f</m:ci>
		<m:ci>t</m:ci>
	      </m:apply>
	    </m:math> has only a finite number of minima and maxima.
	  </item>
	  <item xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
	    In one period, 
	    <m:math>
	      <m:apply>
		<m:ci type="fn">f</m:ci>
		<m:ci>t</m:ci>
	      </m:apply>
	    </m:math> has only a finite number of discontinuities and
	    each one is finite.
	  </item>
	</list>

	These are what we refer to as the <term xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Strong
	Dirichlet Conditions</term>.  In theory we can think of
	signals that violate these conditions,
	<m:math display="inline">
	  <m:apply>
	    <m:sin/>
	    <m:apply>
	      <m:log/>
	      <m:ci>t</m:ci>
	    </m:apply>
	  </m:apply>
	</m:math>
	for instance.  However, it is not possible to create a signal
	that violates these conditions in a lab.  Therefore, any
	real-world signal will have a Fourier representation.
      </para>

		
      <section 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="eg_sub">
	<name xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Example</name>
	<para 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="p1_egs">
	  Let us assume we have the following function and equality:

	  <equation 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="eq_eg1">
	    <m:math>
	      <m:apply>
		<m:eq/>
		<m:apply>
		  <m:diff/>
		  <m:apply>
		    <m:ci type="fn">f</m:ci>
		    <m:ci>t</m:ci>
		  </m:apply>
		</m:apply>
		<m:apply>
		  <m:limit/>
		  <m:bvar>
		    <m:ci>N</m:ci>
		  </m:bvar>
		  <m:lowlimit>
		    <m:infinity/>
		  </m:lowlimit>
		  <m:apply>
		    <m:diff/>
		    <m:apply>
		      <m:ci type="fn">
			<m:msub>
			  <m:mi>f</m:mi>
			  <m:mi>N</m:mi>
			</m:msub>
		      </m:ci>
		      <m:ci>t</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:math>
	  </equation>

	  If 
	  <m:math>
	    <m:apply>
	      <m:ci type="fn">f</m:ci>
	      <m:ci>t</m:ci>
	    </m:apply>
	  </m:math> meets all three conditions of the Strong Dirichlet
	  Conditions, then

	  <m:math display="block">
	    <m:apply>
	      <m:eq/>
	      <m:apply>
		<m:ci type="fn">f</m:ci>
		<m:ci>τ</m:ci>
	      </m:apply>
	      <m:apply>
		<m:diff/>
		<m:apply>
		  <m:ci type="fn">f</m:ci>
		  <m:ci>τ</m:ci>
		</m:apply>
	      </m:apply>
	    </m:apply>
	  </m:math>

	  at every <m:math><m:ci>τ</m:ci></m:math> at which
	   <m:math>
	    <m:apply>
	      <m:ci type="fn">f</m:ci>
	      <m:ci>t</m:ci>
	    </m:apply>
	  </m:math> is continuous.  And where
	  <m:math>
	    <m:apply>
	      <m:ci type="fn">f</m:ci>
	      <m:ci>t</m:ci>
	    </m:apply>
	  </m:math> is discontinuous, 
	   <m:math>
	    <m:apply>
	      <m:diff/>
	      <m:apply>
		<m:ci type="fn">f</m:ci>
		<m:ci>t</m:ci>
	      </m:apply>
	    </m:apply>
	  </m:math> is the <emphasis xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">average</emphasis> of the values
	  on the right and left.  See <cnxn xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" target="figs"/> as an example:
	</para>

	<figure xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" orient="horizontal" id="figs">
	  <subfigure 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="subf1">
	    <media xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" type="image/png" src="dircond1.png"/>
	  </subfigure>
	  <subfigure 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="subf2">
	    <media xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" type="image/png" src="dircond2.png"/>
	  </subfigure>
	  <caption xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">
	    Discontinuous functions, 
	    <m:math>
	      <m:apply>
		<m:ci type="fn">f</m:ci>
		<m:ci>t</m:ci>
	      </m:apply>
	    </m:math>.		      
	  </caption>
	</figure>

	<para 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="pfin">
	  <note xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/" type="note">
	    The functions that fail the Dirchlet conditions are pretty
	    pathological - as engineers, we are not too interested in
	    them. 
	  </note>
	</para>

      </section>

    </section>

  </content>
</document>
