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        <h2>Illustrating wave propagation phenomena</h2>
        
        <p>In this page, I am showing some numerical simulations that I
          completed, mainly during my thesis. These numerical experiments have
          been performed with the software <a href="montjoie/index.php">Montjoie</a>.</p>
        
        <h3> <a href="demo_helmholtz.php">
            Didactic example for solving 2-D Helmholtz equation with finite
            element method</a> </h3>
        
        <table class="center">
          <tr> 
            <td> <a href="demo_helmholtz.php"> <img src="images/TP_SolutionFineMesh.jpg" width="260" height="200" alt="Demo Helmholtz"/> </a>
          </td>
          <td>
            The use of finite element methods is demonstrated for 2-D Helmholtz
            equation. The mesh and solution are generated with the pdetool package
            of Matlab. High-order curved elements are also experimented to show
            their efficiency. </td> </tr>
      </table>
      
      <h3><a href="eigenvalue.php">Eigenvalues for domains presenting a singularity</a></h3>
      
      <table class="center">
        
        <tr> <td> <a href="eigenvalue.php"> <img src="img/ModeLshaped_FirstEy.jpg" width="200" height="200" alt="Eigenvalue computation"/> </a>
         </td>
         <td>
           Benchmark for computing eigenvalues in domains that contain corners or
           singular edges. Nedelec&apos;s edge elements of the first kind are used in
           conjunction with hexahedral mesh with a local refinement.
        </td> </tr>
      </table>
      
      <h3><a href="films/instAvion750.avi">Scattering by an aircraft at 750Mhz</a></h3>
      
      <table class="center"> <tr> <td> <a href="films/instAvion750.avi"> <img src="images/SnapshotAvion750.jpg" width="300" height="200" alt="Diffraction avion"/> </a>
          </td>
          <td>
            A plane wave is scattered by an aircraft. This time-domain
            simulation is performed with Discontinuous Galerkin method on
            hexahedral meshes, and with a local time-stepping strategy.
      </td> </tr> </table>
      
      <h3><a href="films/instAvion900.avi">Scattering by an aircraft at 900Mhz</a></h3>

      <table class="center"> <tr> <td> <a href="films/instAvion900.avi"> <img src="images/SnapshotAvion900.jpg" width="300" height="200" alt="Diffraction avion"/> </a>
          </td>
          <td>
            The same experiment as the previous one is conducted for an higher
            frequency. It can be observed that the mesh seems a bit too coarse for
            this frequency.
      </td> </tr> </table>
      
      <h3> <a href="films/genec.avi"> Scattering by a satellite </a> </h3>

      <table class="center"> <tr> <td> <a href="films/genec.avi"> <img src="images/DiffracGenec.jpg" width="250" height="200" alt="Diffraction Genec"/> </a>
        </td> <td>
          A plane wave is scattered by a satellite (GENEC). The used local time
          stepping strategy is quite efficient on this case because of the
          presence of very small elements (thin slots, solar panels with a small thickness).
      </td> </tr> </table>
      
      <h3><a href="fente/SinusTwiceEps002_L2_F0988_105.avi">
          Resonance phenomena for a finite-length slot.
      </a> </h3>
      
      <table class="center"> <tr> <td> <a href="fente/SinusTwiceEps002_L2_F0988_105.avi">
              <img src="images/DiffracFenteSinus.jpg" width="250" height="200" alt="Diffrac Fente"/> </a>
          </td>
          <td>
            A wave is propagating through a finite-length slot. For some given
            frequencies, some resonances appear and the transmission coefficient
            is higher.
      </td> </tr> </table>
      
      <h3> <a href="fente/RickerEps02_L2.avi"> Propagation of a pulse
          through a slot</a> </h3>

      <table class="center"> <tr> <td> <a href="fente/RickerEps02_L2.avi">
              <img src="images/FenteRickert.jpg" width="120" height="200" alt="Diffrac Fente"/> </a>
          </td>
          <td>
            Propagation of a wave through a slot inside a wall. The time source is
            a Ricker.
      </td> </tr> </table>
      
      <h3> <a href="films/cobra_high.avi">Source point in a cobra cavity</a> </h3>
      
      <table class="center"> <tr> <td> <a href="films/cobra_high.avi">
              <img src="images/SnapshotCobra.jpg" width="260" height="200" alt="Diffrac Cobra"/> </a>
          </td>
          <td>
            A wave is propagating inside a cobra cavity. The right side of the
            cavity is open (numerically a first-order absorbing boundary condition
            is set).
      </td> </tr> </table>
      
      <h3><a href="films/Guide_randomMedia.avi"> Random media in a waveguide</a></h3>
      
      <table class="center"> <tr> <td> <a href="films/Guide_randomMedia.avi">
              <img src="images/GuideRandom.jpg" width="300" height="80" alt="Diffrac guide"/> </a>
          </td>
          <td>
            Propagation of waves inside a waveguide, that is characterized by a
            media with slow random variations. The physical index random variation is
            less than 3%.
      </td> </tr> </table>
      
      <h3><a href="films/BigGuide_randomMedia.avi"> Random media in a big waveguide.</a></h3>

      <table class="center"> <tr> <td> <a href="films/BigGuide_randomMedia.avi">
              <img src="images/BigGuideRandom.jpg" width="250" height="200" alt="Diffrac guide"/> </a>
          </td>
          <td>
            This case is the same as the previous one, but for a larger waveguide
            (500 wavelegnths). The solution is represented by splitting the
            waveguide in several slices.
      </td> </tr> </table>
      
      <h3><a href="atmel/PartAtmel.php">Benchmark of a selective optical filter</a> </h3>
      
      <table class="center"> <tr> <td> <a href="atmel/PartAtmel.php">
              <img src="atmel/D40W10CourbeReson.jpg" width="200" height="200" alt="Benchmark Atmel"/></a>
          </td>
          <td>
            Studying an optical band-pass filter. This filter is highly
            selective, and this sensitivity is favorable to high-order element methods.
      </td> </tr> </table>
      
      <h3><a href="films/FilExact.avi"> Scattering of a plane wave by a thin
          wire</a> </h3>
      
      <table class="center"> <tr> <td> <a href="films/FilExact.avi">
              <img src="images/ChampTotalWire_Eps002_T3.jpg" width="200" height="200" alt="Diffrac Fil"/> </a>
          </td>
          <td>
            Electromagnetic waves are scattered by a thin wire. Several models are
            available (Holland's model, fictitious domain model)
      </td> </tr> </table>
      
      <table class="center"> <tr> <td> <a href="films/AeroSphere.avi">
              <img src="images/AeroSphere.jpg" width="300" height="200" alt="Aero sphere"/> </a>
          </td>
          <td>
            Propagation of an acoustic wave in presence of a flow. 
            Solving Linearized Euler equations with Discontinuous Galerkin method
            with hexahedral mesh.
      </td> </tr> </table>
      
      <table class="center"> <tr> <td> <a href="films/PianoSurf.avi">
              <img src="images/MaillagePianoHybrid.jpg" width="300" height="200" alt="Piano diffrac"/> </a>
          </td>
          <td>
            Propagation of an acoustic wave inside a piano-shaped cavity.
      </td> </tr> </table>
      
      <table class="center"> <tr> <td> <a href="films/PropagationLung.avi">
              <img src="images/SnapshotLung.jpg" width="300" height="200" alt="Lung diffrac"/> </a>
          </td>
          <td>
            Propagation of an acoustic wave inside the lungs.
      </td> </tr> </table>
      
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