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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/">Fourier Analysis</name>

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      <md:firstname xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Richard</md:firstname>
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    <md:keyword xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">continuous time</md:keyword>
    <md:keyword xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">discrete time</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>
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    <md:keyword xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">z transform</md:keyword>
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  <md:abstract xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Lists the four Fourier transforms and when to use them.</md:abstract>
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    <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="para1">
      Fourier analysis is fundamental to understanding the behavior of
      signals and systems.  This is a result of the fact that
      sinusoids are <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/" strength="5" document="m10500">Eigenfunctions</cnxn> of <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/" strength="5" document="m10084">linear, time-invariant (LTI)</cnxn> systems.
      This is to say that if we pass any particular sinusoid through a
      LTI system, we get a scaled version of that same sinusoid on the
      output.  Then, since Fourier analysis allows us to redefine the
      signals in terms of sinusoids, all we need to do is determine
      how any given system effects all possible sinusoids (its <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/" strength="5" document="m0028">transfer function</cnxn>) and we
      have a complete understanding of the system.  Furthermore, since
      we are able to define the passage of sinusoids through a system
      as multiplication of that sinusoid by the transfer function at
      the same frequency, we can convert the passage of any signal
      through a system from <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/" strength="5" document="m10088">convolution</cnxn> (in time) to multiplication
      (in frequency).  These ideas are what give Fourier analysis its
      power.
    </para>
    <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="para2">
      Now, after hopefully having sold you on the value of this method
      of analysis, we must examine exactly what we mean by Fourier
      analysis.  The four Fourier transforms that comprise this
      analysis are 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/" strength="5" document="m10097">Fourier
      Series</cnxn>, <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/" strength="5" document="m10098">Continuous-Time Fourier Transform</cnxn>,
      <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/" strength="5" document="m10108">Discrete-Time Fourier
      Transform</cnxn> and <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/" strength="5" document="m0502">Discrete Fourier Transform</cnxn>.  For this
      document, we will view 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/" strength="5" document="m10110">Laplace Transform</cnxn> and <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/" strength="5" document="m10119">Z-Transform</cnxn> as simply
      extensions of the CTFT and DTFT respectively.  All of these
      transforms act essentially the same way, by converting a signal
      in time to an equivalent signal in frequency (sinusoids).
      However, depending on the nature of a specific signal
      <foreign xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">i.e.</foreign> whether it is finite- or infinite-length
      and whether it is discrete- or continuous-time) there is an
      appropriate transform to convert the signal into the frequency
      domain.  Below is a table of the four Fourier transforms and
      when each is appropriate.  It also includes the relevant
      convolution for the specified space.
    </para>
    
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	    <entry xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Continuous-Time Circular</entry>
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	    <entry xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Discrete-Time Fourier Transform</entry>
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	    <entry xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:bib="http://bibtexml.sf.net/">Discrete-Time Circular</entry>
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