<?xml version='1.0' encoding='UTF-8'?><?xml-stylesheet href="http://www.blogger.com/styles/atom.css" type="text/css"?><feed xmlns='http://www.w3.org/2005/Atom' xmlns:openSearch='http://a9.com/-/spec/opensearchrss/1.0/' xmlns:georss='http://www.georss.org/georss' xmlns:gd='http://schemas.google.com/g/2005' xmlns:thr='http://purl.org/syndication/thread/1.0'><id>tag:blogger.com,1999:blog-7735848022985100293</id><updated>2012-02-16T04:41:01.174-08:00</updated><category term='September Sunday at the village'/><title type='text'>Toulopoulos Ioannis</title><subtitle type='html'>Mathematician</subtitle><link rel='http://schemas.google.com/g/2005#feed' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/posts/default'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default?max-results=100'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/'/><link rel='hub' href='http://pubsubhubbub.appspot.com/'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><generator version='7.00' uri='http://www.blogger.com'>Blogger</generator><openSearch:totalResults>12</openSearch:totalResults><openSearch:startIndex>1</openSearch:startIndex><openSearch:itemsPerPage>100</openSearch:itemsPerPage><entry><id>tag:blogger.com,1999:blog-7735848022985100293.post-7183857868445388359</id><published>2009-12-07T10:59:00.000-08:00</published><updated>2009-12-07T07:03:12.344-08:00</updated><title type='text'>Home</title><content type='html'>&lt;a href="http://toulio.blogspot.com"&gt; Click here to return Home &lt;/a&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7735848022985100293-7183857868445388359?l=toulio.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/7183857868445388359/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://toulio.blogspot.com/2009/06/home_17.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/7183857868445388359'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/7183857868445388359'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/2009/06/home_17.html' title='Home'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-7735848022985100293.post-9120223723993952121</id><published>2009-12-05T09:55:00.000-08:00</published><updated>2009-12-07T07:03:37.416-08:00</updated><title type='text'>Research Interests</title><content type='html'>&lt;meta equiv="Content-Type" content="text/html; 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&lt;/style&gt;&lt;!--[if gte mso 10]&gt; &lt;style&gt;  /* Style Definitions */  table.MsoNormalTable 	{mso-style-name:"Κανονικός πίνακας"; 	mso-tstyle-rowband-size:0; 	mso-tstyle-colband-size:0; 	mso-style-noshow:yes; 	mso-style-parent:""; 	mso-padding-alt:0cm 5.4pt 0cm 5.4pt; 	mso-para-margin:0cm; 	mso-para-margin-bottom:.0001pt; 	mso-pagination:widow-orphan; 	font-size:10.0pt; 	font-family:"Times New Roman"; 	mso-ansi-language:#0400; 	mso-fareast-language:#0400; 	mso-bidi-language:#0400;} &lt;/style&gt; &lt;![endif]--&gt;  &lt;p class="1" style="margin: 0cm -2.15pt 6pt 0cm; text-align: justify;"&gt;&lt;span style="font-size: 12pt; font-family: &amp;quot;Times New Roman&amp;quot;;"&gt;Numerical solution of&lt;span style=""&gt;  &lt;/span&gt;PDE’s. Computational fluid dynamics: finite element schemes for hyperbolic problems, design of new finite element schemes for &lt;span style=""&gt; &lt;/span&gt;hyperbolic conservation laws&lt;span style=""&gt;  &lt;/span&gt;with time dependent &lt;span style=""&gt; &lt;/span&gt;boundary conditions, strong wave interactions, shocks, complex viscous flow features, flows in the presence of magnetic fields. &lt;o:p&gt;&lt;/o:p&gt;&lt;/span&gt;&lt;/p&gt;  &lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7735848022985100293-9120223723993952121?l=toulio.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/9120223723993952121/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://toulio.blogspot.com/2009/06/research-interests_15.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/9120223723993952121'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/9120223723993952121'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/2009/06/research-interests_15.html' title='Research Interests'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-7735848022985100293.post-1920092103113130679</id><published>2009-12-05T06:12:00.000-08:00</published><updated>2009-12-07T07:16:57.752-08:00</updated><title type='text'>Graphs DG, Aeroacoustic Problems</title><content type='html'>Radiation Boundary Conditions, Characteristic Boundary Conditions&lt;br /&gt;&lt;span class="fullpost"&gt; &lt;br /&gt;&lt;p&gt;Time harmonic source problem - Scattering by cylinder surface. &lt;br /&gt;The computed pressure field using P3 local space and characteristic boundary conditions at the far field boundary part, see mypaper[3j].&lt;p&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://1.bp.blogspot.com/_paT6dlY5x_g/SmDMM0k7I_I/AAAAAAAAAD4/y4aMV-WsiBA/s1600-h/TimHarSrc.jpg"&gt;&lt;img style="cursor:pointer; cursor:hand;width: 320px; height: 182px;" src="http://1.bp.blogspot.com/_paT6dlY5x_g/SmDMM0k7I_I/AAAAAAAAAD4/y4aMV-WsiBA/s320/TimHarSrc.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5359508077214901234" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;p&gt;Acoustic pulse scattering by a cylinder surface. &lt;br /&gt;The computed pressure field using P&lt;/sup&gt;3&lt;/sup&gt; local polynomial space and &lt;br /&gt;characteristic boundary conditions at the boundaries, see my paper [3j].&lt;br&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://1.bp.blogspot.com/_paT6dlY5x_g/SmDLuWqVZBI/AAAAAAAAADw/vg7Ii2z28z0/s1600-h/Puls_Aer_1.jpg"&gt;&lt;img style="cursor:pointer; cursor:hand;width: 320px; height: 224px;" src="http://1.bp.blogspot.com/_paT6dlY5x_g/SmDLuWqVZBI/AAAAAAAAADw/vg7Ii2z28z0/s320/Puls_Aer_1.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5359507553788453906" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;p&gt;&lt;br /&gt;Time harmonic source problem. Left: the pressure computed field using P3 local space  using characteristic boundary conditions, Right: the variation of the L2 error measured on the boundary elements at every time step.&lt;br&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SmDOHf2PzEI/AAAAAAAAAEI/z2K51TCCQaQ/s1600-h/Aer_HarsrcL2TmCH_2.jpg"&gt;&lt;img style="cursor:pointer; cursor:hand;width: 320px; height: 154px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SmDOHf2PzEI/AAAAAAAAAEI/z2K51TCCQaQ/s320/Aer_HarsrcL2TmCH_2.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5359510184774323266" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;p&gt;&lt;br /&gt;Propagation and reflection from a solid wall of an acoustic pulse. &lt;br /&gt;The compute pressure field using radiation boundary conditions at the far field boundary parts. &lt;br&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SmDMvduzXyI/AAAAAAAAAEA/zkiCOOj3HH8/s1600-h/Aer_PulsSoWal_RDBC_3.jpg"&gt;&lt;img style="cursor:pointer; cursor:hand;width: 320px; height: 169px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SmDMvduzXyI/AAAAAAAAAEA/zkiCOOj3HH8/s320/Aer_PulsSoWal_RDBC_3.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5359508672377741090" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7735848022985100293-1920092103113130679?l=toulio.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/1920092103113130679/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://toulio.blogspot.com/2009/06/graphs-dg-numerical-solutions_5011.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/1920092103113130679'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/1920092103113130679'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/2009/06/graphs-dg-numerical-solutions_5011.html' title='Graphs DG, Aeroacoustic Problems'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><media:thumbnail xmlns:media='http://search.yahoo.com/mrss/' url='http://1.bp.blogspot.com/_paT6dlY5x_g/SmDMM0k7I_I/AAAAAAAAAD4/y4aMV-WsiBA/s72-c/TimHarSrc.jpg' height='72' width='72'/><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-7735848022985100293.post-5330489640607909208</id><published>2009-12-04T11:48:00.000-08:00</published><updated>2009-12-07T07:04:32.084-08:00</updated><title type='text'>Graphs DG,  Nonlinear Euler, Problems with Smooth Solutions</title><content type='html'>Steady state solutions, flow past over a cylinder&lt;br /&gt;&lt;span class="fullpost"&gt; &lt;br /&gt;Flow past over a cylinder, the Mach number computed field using P5 local polynomial space. The cylinder surface is descritized using 90 elelements. &lt;p&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://1.bp.blogspot.com/_paT6dlY5x_g/SmDKXCTmhWI/AAAAAAAAADo/tkjt839loKg/s1600-h/FLCyl_P5sp_5.jpg"&gt;&lt;img style="cursor:pointer; cursor:hand;width: 320px; height: 306px;" src="http://1.bp.blogspot.com/_paT6dlY5x_g/SmDKXCTmhWI/AAAAAAAAADo/tkjt839loKg/s320/FLCyl_P5sp_5.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5359506053675779426" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7735848022985100293-5330489640607909208?l=toulio.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/5330489640607909208/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://toulio.blogspot.com/2009/07/graphs-dg-nonlinear-euler-problems-with.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/5330489640607909208'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/5330489640607909208'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/2009/07/graphs-dg-nonlinear-euler-problems-with.html' title='Graphs DG,  Nonlinear Euler, Problems with Smooth Solutions'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><media:thumbnail xmlns:media='http://search.yahoo.com/mrss/' url='http://1.bp.blogspot.com/_paT6dlY5x_g/SmDKXCTmhWI/AAAAAAAAADo/tkjt839loKg/s72-c/FLCyl_P5sp_5.jpg' height='72' width='72'/><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-7735848022985100293.post-2019215676208314632</id><published>2009-12-04T09:51:00.000-08:00</published><updated>2009-12-07T07:04:50.620-08:00</updated><title type='text'>Grpahs DG, Compressible Navier Stokes</title><content type='html'>Flow past over a cylinder&lt;br /&gt;&lt;span class="fullpost"&gt;&lt;br /&gt;&lt;br /&gt;DG numerical solution of the viscous flow problem (flow past over a cylinder) using characteristic boundary conditions at the outflow boundary part of the computational domain, (toulio 2009, see mypaper 3j)&lt;p&gt;&lt;br /&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SjvDXF0VelI/AAAAAAAAACo/yL8a99Kv1IY/s1600-h/NS_web.jpg"&gt;&lt;img style="cursor:pointer; cursor:hand;width: 320px; height: 255px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SjvDXF0VelI/AAAAAAAAACo/yL8a99Kv1IY/s320/NS_web.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5349083783898692178" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7735848022985100293-2019215676208314632?l=toulio.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/2019215676208314632/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://toulio.blogspot.com/2009/06/new.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/2019215676208314632'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/2019215676208314632'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/2009/06/new.html' title='Grpahs DG, Compressible Navier Stokes'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><media:thumbnail xmlns:media='http://search.yahoo.com/mrss/' url='http://3.bp.blogspot.com/_paT6dlY5x_g/SjvDXF0VelI/AAAAAAAAACo/yL8a99Kv1IY/s72-c/NS_web.jpg' height='72' width='72'/><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-7735848022985100293.post-5976212204015341404</id><published>2009-12-04T09:23:00.000-08:00</published><updated>2009-12-07T07:05:09.923-08:00</updated><title type='text'>Graphs DG, Nonlinear Euler Equations Discontinuous Solutions</title><content type='html'>Double Forward Facing Step, Double Mach Reflection&lt;br&gt;&lt;br /&gt;&lt;span class="fullpost"&gt;&lt;br /&gt;A new shock capturing scheme, using extrema control conditions (toulio 2009, see mypaper 8c)&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;  &lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ2cPm6J_I/AAAAAAAAABo/Wel6d5c3FOU/s1600-h/Fwp1_frs_P1_100.jpg"&gt;&lt;img style="float:left; margin:0 10px 10px 0;cursor:pointer; cursor:hand;width: 320px; height: 130px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ2cPm6J_I/AAAAAAAAABo/Wel6d5c3FOU/s320/Fwp1_frs_P1_100.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5347591835147184114" /&gt;&lt;/a&gt; &lt;p&gt;&lt;br /&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://2.bp.blogspot.com/_paT6dlY5x_g/SjZ2mBVhqEI/AAAAAAAAABw/admjWotBTtQ/s1600-h/Fwp2_fr3msh_p2.jpg"&gt;&lt;img style="float:left; margin:0 10px 10px 0;cursor:pointer; cursor:hand;width: 320px; height: 258px;" src="http://2.bp.blogspot.com/_paT6dlY5x_g/SjZ2mBVhqEI/AAAAAAAAABw/admjWotBTtQ/s320/Fwp2_fr3msh_p2.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5347592003114870850" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ3pFZO8II/AAAAAAAAAB4/hMRJoybv1j4/s1600-h/Fwp3_DMR_p1_160.jpg"&gt;&lt;img style="float:left; margin:0 10px 10px 0;cursor:pointer; cursor:hand;width: 320px; height: 126px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ3pFZO8II/AAAAAAAAAB4/hMRJoybv1j4/s320/Fwp3_DMR_p1_160.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5347593155255398530" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ32047EPI/AAAAAAAAACA/a328qUgerUg/s1600-h/Fwp3_DMR_p2_160.jpg"&gt;&lt;img style="float:left; margin:0 10px 10px 0;cursor:pointer; cursor:hand;width: 320px; height: 126px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ32047EPI/AAAAAAAAACA/a328qUgerUg/s320/Fwp3_DMR_p2_160.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5347593391343079666" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7735848022985100293-5976212204015341404?l=toulio.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/5976212204015341404/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://toulio.blogspot.com/2009/06/graphs-nonlinear-euler-equations.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/5976212204015341404'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/5976212204015341404'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/2009/06/graphs-nonlinear-euler-equations.html' title='Graphs DG, Nonlinear Euler Equations Discontinuous Solutions'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><media:thumbnail xmlns:media='http://search.yahoo.com/mrss/' url='http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ2cPm6J_I/AAAAAAAAABo/Wel6d5c3FOU/s72-c/Fwp1_frs_P1_100.jpg' height='72' width='72'/><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-7735848022985100293.post-616769330803991386</id><published>2009-12-04T08:55:00.000-08:00</published><updated>2009-12-08T06:32:17.572-08:00</updated><title type='text'>3D Graphs DG, Nonlinear Euler equations</title><content type='html'>Steady state solutions, flow past over a cylinder&lt;br /&gt;&lt;span class="fullpost"&gt; &lt;br /&gt;Steady state flow problems, flow past over a cylinder. &lt;br /&gt;The subdivision of the  3 Dimensional computational domain by tetrahedral elements. The surface of the cylinder has been discretised  using 20   elements&lt;br /&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://1.bp.blogspot.com/_paT6dlY5x_g/Sx0d1xGevQI/AAAAAAAAAEw/RwSt4lqf16c/s1600-h/3D_Domain.jpg"&gt;&lt;img style="display:block; margin:0px auto 10px; text-align:center;cursor:pointer; cursor:hand;width: 320px; height: 244px;" src="http://1.bp.blogspot.com/_paT6dlY5x_g/Sx0d1xGevQI/AAAAAAAAAEw/RwSt4lqf16c/s320/3D_Domain.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5412515136719994114" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;The Mach number computed field using P1 local polynomial space. Simple extrapolated inflow – outflow boundary conditions have been implemented. &lt;br /&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/Sx0du9FAoyI/AAAAAAAAAEo/zSCPw_skkvE/s1600-h/MachField.jpg"&gt;&lt;img style="display:block; margin:0px auto 10px; text-align:center;cursor:pointer; cursor:hand;width: 320px; height: 244px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/Sx0du9FAoyI/AAAAAAAAAEo/zSCPw_skkvE/s320/MachField.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5412515019675968290" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://2.bp.blogspot.com/_paT6dlY5x_g/Sx0dhyzbItI/AAAAAAAAAEg/virR-PX2Q8g/s1600-h/3D_Inflow.jpg"&gt;&lt;img style="display:block; margin:0px auto 10px; text-align:center;cursor:pointer; cursor:hand;width: 320px; height: 244px;" src="http://2.bp.blogspot.com/_paT6dlY5x_g/Sx0dhyzbItI/AAAAAAAAAEg/virR-PX2Q8g/s320/3D_Inflow.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5412514793579553490" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/Sx5jYv5YBsI/AAAAAAAAAE4/JtYFYiZWf3M/s1600-h/MacFLD_fl.jpg"&gt;&lt;img style="display:block; margin:0px auto 10px; text-align:center;cursor:pointer; cursor:hand;width: 320px; height: 284px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/Sx5jYv5YBsI/AAAAAAAAAE4/JtYFYiZWf3M/s320/MacFLD_fl.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5412873078971041474" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7735848022985100293-616769330803991386?l=toulio.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/616769330803991386/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://toulio.blogspot.com/2009/12/3d-graphs-dg-nonlinear-euler-equations.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/616769330803991386'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/616769330803991386'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/2009/12/3d-graphs-dg-nonlinear-euler-equations.html' title='3D Graphs DG, Nonlinear Euler equations'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><media:thumbnail xmlns:media='http://search.yahoo.com/mrss/' url='http://1.bp.blogspot.com/_paT6dlY5x_g/Sx0d1xGevQI/AAAAAAAAAEw/RwSt4lqf16c/s72-c/3D_Domain.jpg' height='72' width='72'/><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-7735848022985100293.post-3545121824943406526</id><published>2009-12-04T08:40:00.000-08:00</published><updated>2009-12-07T07:16:10.080-08:00</updated><title type='text'>Graphs of Numerical Solutions of  Benchmark problems</title><content type='html'>&lt;span class="fullpost"&gt; &lt;br /&gt;&lt;a name="top"&gt;&lt;/a&gt;&lt;br /&gt;&lt;ol&gt;&lt;br /&gt;&lt;li type=disk&gt; &lt;a href="#Graph1"&gt;Graphs DG, Nonlinear Euler, Problems with Smooth Solutions&lt;/a&gt;&lt;br /&gt;Steady state solutions, flow past over a cylinder&lt;br /&gt;&lt;li type=disk&gt;&lt;a href="#Graph2"&gt;Graphs DG, Compressible Navier Stokes&lt;br&gt;Flow past over a cylinder&lt;/a&gt;&lt;br /&gt;&lt;li type=disk&gt; &lt;a href="#Graph3"&gt;Graphs DG, Nonlinear Euler Equations Discontinuous Solutions&lt;br&gt;Double Forward Facing Step, Double Mach Reflection&lt;/a&gt;&lt;br /&gt;&lt;li type=disk&gt;&lt;a href="#Graph4"&gt;Graphs DG, Aeroacoustic Problems&lt;br /&gt;Radiation Boundary Conditions, Characteristic Boundary Conditions&lt;/a&gt;&lt;br /&gt;&lt;/ol&gt;&lt;br /&gt;&lt;br /&gt;&lt;ol&gt;&lt;br /&gt;&lt;a name="Graph1"&gt;&lt;/a&gt;&lt;br /&gt;&lt;li type=disk&gt;&lt;b&gt;Graphs DG, Nonlinear Euler, Problems with Smooth Solutions &lt;/b&gt;&lt;br /&gt;Steady state solutions, flow past over a cylinder&lt;br&gt;&lt;br /&gt;Flow past over a cylinder, the Mach number computed field using P5 local polynomial space. The cylinder surface is descritized using 90 elelements. &lt;p&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://1.bp.blogspot.com/_paT6dlY5x_g/SmDKXCTmhWI/AAAAAAAAADo/tkjt839loKg/s1600-h/FLCyl_P5sp_5.jpg"&gt;&lt;img style="cursor:pointer; cursor:hand;width: 320px; height: 306px;" src="http://1.bp.blogspot.com/_paT6dlY5x_g/SmDKXCTmhWI/AAAAAAAAADo/tkjt839loKg/s320/FLCyl_P5sp_5.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5359506053675779426" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;a href="#top"&gt;[Top]&lt;/a&gt;&lt;br /&gt;&lt;a name="Graph2"&gt;&lt;/a&gt;&lt;br /&gt;&lt;li type=disk&gt;&lt;b&gt;Graphs DG, Compressible Navier Stokes&lt;/b&gt;&lt;br&gt;Flow past over a cylinder&lt;br&gt;&lt;br /&gt;DG numerical solution of the viscous flow problem (flow past over a cylinder) using characteristic boundary conditions at the outflow boundary part of the computational domain, (toulio 2009, see mypaper 3j)&lt;p&gt;&lt;br /&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SjvDXF0VelI/AAAAAAAAACo/yL8a99Kv1IY/s1600-h/NS_web.jpg"&gt;&lt;img style="cursor:pointer; cursor:hand;width: 320px; height: 255px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SjvDXF0VelI/AAAAAAAAACo/yL8a99Kv1IY/s320/NS_web.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5349083783898692178" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;a href="#top"&gt;[Top]&lt;/a&gt;&lt;br /&gt;&lt;a name="Graph3"&gt;&lt;/a&gt;&lt;br /&gt;&lt;li type=disk&gt;&lt;b&gt;Graphs DG, Nonlinear Euler Equations Discontinuous Solutions&lt;/b&gt;&lt;br&gt;Double Forward Facing Step, Double Mach Reflection&lt;br&gt;&lt;br /&gt;A new shock capturing scheme, using extrema control conditions (toulio 2009, see mypaper 8c)&lt;br /&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ2cPm6J_I/AAAAAAAAABo/Wel6d5c3FOU/s1600-h/Fwp1_frs_P1_100.jpg"&gt;&lt;img style="float:left; margin:0 10px 10px 0;cursor:pointer; cursor:hand;width: 320px; height: 130px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ2cPm6J_I/AAAAAAAAABo/Wel6d5c3FOU/s320/Fwp1_frs_P1_100.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5347591835147184114" /&gt;&lt;/a&gt; &lt;p&gt;&lt;br /&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://2.bp.blogspot.com/_paT6dlY5x_g/SjZ2mBVhqEI/AAAAAAAAABw/admjWotBTtQ/s1600-h/Fwp2_fr3msh_p2.jpg"&gt;&lt;img style="float:left; margin:0 10px 10px 0;cursor:pointer; cursor:hand;width: 320px; height: 258px;" src="http://2.bp.blogspot.com/_paT6dlY5x_g/SjZ2mBVhqEI/AAAAAAAAABw/admjWotBTtQ/s320/Fwp2_fr3msh_p2.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5347592003114870850" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ3pFZO8II/AAAAAAAAAB4/hMRJoybv1j4/s1600-h/Fwp3_DMR_p1_160.jpg"&gt;&lt;img style="float:left; margin:0 10px 10px 0;cursor:pointer; cursor:hand;width: 320px; height: 126px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ3pFZO8II/AAAAAAAAAB4/hMRJoybv1j4/s320/Fwp3_DMR_p1_160.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5347593155255398530" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ32047EPI/AAAAAAAAACA/a328qUgerUg/s1600-h/Fwp3_DMR_p2_160.jpg"&gt;&lt;img style="float:left; margin:0 10px 10px 0;cursor:pointer; cursor:hand;width: 320px; height: 126px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ32047EPI/AAAAAAAAACA/a328qUgerUg/s320/Fwp3_DMR_p2_160.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5347593391343079666" /&gt;&lt;/a&gt;&lt;p&gt;&lt;br /&gt;&lt;br /&gt;&lt;a href="#top"&gt;[Top]&lt;/a&gt;&lt;br /&gt;&lt;a name="Graph4"&gt;&lt;/a&gt;&lt;br /&gt;&lt;li type=disk&gt;&lt;b&gt;Graphs DG, Aeroacoustic Problems&lt;br&gt;Radiation Boundary Conditions, Characteristic Boundary Conditions&lt;/b&gt;&lt;br&gt;&lt;br /&gt;&lt;/ol&gt;&lt;br /&gt;&lt;p&gt;Time harmonic source problem - Scattering by cylinder surface. &lt;br /&gt;The computed pressure field using P3 local space and characteristic boundary conditions at the far field boundary part, see mypaper[3j].&lt;p&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://1.bp.blogspot.com/_paT6dlY5x_g/SmDMM0k7I_I/AAAAAAAAAD4/y4aMV-WsiBA/s1600-h/TimHarSrc.jpg"&gt;&lt;img style="cursor:pointer; cursor:hand;width: 320px; height: 182px;" src="http://1.bp.blogspot.com/_paT6dlY5x_g/SmDMM0k7I_I/AAAAAAAAAD4/y4aMV-WsiBA/s320/TimHarSrc.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5359508077214901234" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;p&gt;Acoustic pulse scattering by a cylinder surface. &lt;br /&gt;The computed pressure field using P&lt;/sup&gt;3&lt;/sup&gt; local polynomial space and &lt;br /&gt;characteristic boundary conditions at the boundaries, see my paper [3j].&lt;br&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://1.bp.blogspot.com/_paT6dlY5x_g/SmDLuWqVZBI/AAAAAAAAADw/vg7Ii2z28z0/s1600-h/Puls_Aer_1.jpg"&gt;&lt;img style="cursor:pointer; cursor:hand;width: 320px; height: 224px;" src="http://1.bp.blogspot.com/_paT6dlY5x_g/SmDLuWqVZBI/AAAAAAAAADw/vg7Ii2z28z0/s320/Puls_Aer_1.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5359507553788453906" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;p&gt;&lt;br /&gt;Time harmonic source problem. Left: the pressure computed field using P3 local space  using characteristic boundary conditions, Right: the variation of the L2 error measured on the boundary elements at every time step.&lt;br&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SmDOHf2PzEI/AAAAAAAAAEI/z2K51TCCQaQ/s1600-h/Aer_HarsrcL2TmCH_2.jpg"&gt;&lt;img style="cursor:pointer; cursor:hand;width: 320px; height: 154px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SmDOHf2PzEI/AAAAAAAAAEI/z2K51TCCQaQ/s320/Aer_HarsrcL2TmCH_2.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5359510184774323266" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;p&gt;&lt;br /&gt;Propagation and reflection from a solid wall of an acoustic pulse. &lt;br /&gt;The compute pressure field using radiation boundary conditions at the far field boundary parts. &lt;br&gt;&lt;br /&gt;&lt;a onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SmDMvduzXyI/AAAAAAAAAEA/zkiCOOj3HH8/s1600-h/Aer_PulsSoWal_RDBC_3.jpg"&gt;&lt;img style="cursor:pointer; cursor:hand;width: 320px; height: 169px;" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SmDMvduzXyI/AAAAAAAAAEA/zkiCOOj3HH8/s320/Aer_PulsSoWal_RDBC_3.jpg" border="0" alt=""id="BLOGGER_PHOTO_ID_5359508672377741090" /&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;a href="#top"&gt;[Top]&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7735848022985100293-3545121824943406526?l=toulio.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/3545121824943406526/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://toulio.blogspot.com/2009/11/graphs.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/3545121824943406526'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/3545121824943406526'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/2009/11/graphs.html' title='Graphs of Numerical Solutions of  Benchmark problems'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><media:thumbnail xmlns:media='http://search.yahoo.com/mrss/' url='http://1.bp.blogspot.com/_paT6dlY5x_g/SmDKXCTmhWI/AAAAAAAAADo/tkjt839loKg/s72-c/FLCyl_P5sp_5.jpg' height='72' width='72'/><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-7735848022985100293.post-4063402086432520266</id><published>2009-12-04T07:40:00.000-08:00</published><updated>2009-12-07T07:11:06.270-08:00</updated><title type='text'>Synopsis of Dessertation</title><content type='html'>&lt;a href='http://groups.google.com/group/ioantlp/web/toulioDisert.pdf?hl=en-GB'&gt;Synopsis of Dessertation&lt;/a&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7735848022985100293-4063402086432520266?l=toulio.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/4063402086432520266/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://toulio.blogspot.com/2009/07/synopsis-of-dessertation.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/4063402086432520266'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/4063402086432520266'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/2009/07/synopsis-of-dessertation.html' title='Synopsis of Dessertation'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-7735848022985100293.post-264765399975556938</id><published>2009-12-04T03:39:00.000-08:00</published><updated>2009-12-07T07:06:00.155-08:00</updated><title type='text'>Curriculum Vitae</title><content type='html'>&lt;a href='http://groups.google.com/group/ioantlp/web/CV_toulopoulos.doc.pdf?hl=el'&gt;Download my CV&lt;/a&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7735848022985100293-264765399975556938?l=toulio.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/264765399975556938/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://toulio.blogspot.com/2009/06/curriculum-vitae.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/264765399975556938'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/264765399975556938'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/2009/06/curriculum-vitae.html' title='Curriculum Vitae'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-7735848022985100293.post-5282054784563635973</id><published>2009-12-03T10:35:00.000-08:00</published><updated>2010-03-20T06:43:04.523-07:00</updated><title type='text'>My Papers</title><content type='html'>&lt;span class="fullpost"&gt;&lt;span style="font-weight: bold;"&gt;Papers in journals&lt;/span&gt;&lt;br /&gt;&lt;span style="font-weight: bold;font-size:130%;" &gt;&lt;a href="http://groups.google.com/group/ioantlp/web/AIAAchbc.pdf?hl=en"&gt;1j. &lt;/span&gt;I. Toulopoulos and J. A. Ekaterinaris  ‘High-Order Discontinuous Galerkin Discretizations for Computational Aeroacoustics in Complex Domains’, AIAA Journal, Vol. 44, No. 3, 2006, pp. 502-511.&lt;/a&gt;&lt;p&gt;&lt;br /&gt;&lt;span style="font-weight: bold;font-size:130%;" &gt;2j. &lt;/span&gt;G. Arabatzis, P. Vavilis, I. Toulopoulos and J. A. Ekaterinaris, ‘Implicit High-Order Time-Marching Schemes for the Linearized Euler Equations’ AIAA Journal, Vol. 45, No. 8,&lt;br /&gt;2007, pp 1819-1826.&lt;p&gt;&lt;br /&gt;   &lt;span style="font-weight: bold;font-size:130%;" &gt;3j.&lt;/span&gt;&lt;span style="font-size:130%;"&gt;  &lt;/span&gt;I. Toulopoulos and J. A. Ekaterinaris ‘Artificial boundary conditions for the numerical&lt;br /&gt;         solution of the Euler equations by the discontinuous Galerkin finite element method’&lt;br /&gt;         submitted to a journal.&lt;br /&gt;&lt;br /&gt;&lt;span style="font-weight: bold;font-size:130%;" &gt;4j&lt;/span&gt; I. Toulopoulos and C. Makridakis "A  new discontinuous Galerkin  scheme for the numerical solution of flow problems with discontinuities"&lt;br /&gt;submitted for publishing&lt;br /&gt;                   &lt;br /&gt;         &lt;span style="font-weight: bold;"&gt;Papers in conferences &lt;/span&gt;&lt;br /&gt;&lt;span style="font-weight: bold;font-size:130%;" &gt;&lt;a href="http://groups.google.com/group/ioantlp/web/AIAA-2003_DGNS.pdf?hl=en"&gt;3c.  &lt;/span&gt;I. Toulopoulos and J. A. Ekaterinaris ‘Discontinuous Galerkin Discretizations for Viscous        Flow Problems in Complex Domains’, 43th AIAA Aerospace Science Meeting and Exhibit, 10-13 Jan. 2005, Reno-Nevada, USA AIAA paper 1265.&lt;/a&gt;&lt;br /&gt;&lt;span style="font-weight: bold;"&gt;&lt;a href"http://groups.google.com/group/ioantlp/web/ToronJ2006.pdf?hl=en"&gt;4c.&lt;/span&gt; I. Toulopoulos and J. A. Ekaterinaris ‘High resolution Compressible flow Simulations with the discontinuous Galerkin Method’, 17th  AIAA Computational Fluid Dynamics Conference,  6-9 June 2005, Toronto Canada, AIAA paper 5109.&lt;/a&gt;&lt;br /&gt;&lt;span style="font-weight: bold;font-size:130%;" &gt;5c.&lt;/span&gt; I. Toulopoulos and J. A. Ekaterinaris ‘Implementation of Characteristic boundary conditions to the discontinuous Galerkin Method’, 44th AIAA Aerospace Science Meeting and Exhibit, 9-12 Jan. 2006, Reno-Nevada, USA AIAA paper 0108.&lt;br /&gt;&lt;span style="font-size:130%;"&gt;&lt;span style="font-weight: bold;"&gt;6c.&lt;/span&gt;&lt;/span&gt; I. Toulopoulos and J. A. Ekaterinaris ‘High order shock capturing discontinuous Galerkin schemes’ Proceedings of European Conference on Computational Fluid Dynamics,  5-8  September 2006, Egmond aan Zee, Holland, editors P. wasseling, E. Onate, J. Periaux.&lt;br /&gt;&lt;span style="font-size:130%;"&gt;&lt;span style="font-weight: bold;"&gt;7c.&lt;/span&gt;&lt;/span&gt; I. Toulopoulos and J. A. Ekaterinaris ‘On the Application of Filters for Discontinuity Capturing with High Order Discontinuous Galerkin Discritizations’ International Workshop on High-order Finite Element Methods, 17-19 May 2007,  Herrsching am Ammersee (near Munich), Germany.&lt;br /&gt;&lt;span style="font-weight: bold;font-size:130%;" &gt;8c.&lt;/span&gt; I. Toulopoulos and C. Makridakis ‘A discontinuous Galerkin shock-capturing scheme for the numerical solution of compressible flow problems’, Proceeding of Conference in Numerical Analysis (NumAn 2008), pages 195-200, 1-5 September 2008, Kalamata Greece, editors G. Akrivis,E. Gallopoulos,  A. Hadjidimos, I. S. Kotsireas, D. Noutsos, M. N. Vrahatis.&lt;br /&gt;&lt;br /&gt;&lt;p&gt;&lt;br /&gt;&lt;b&gt;Other reserch contributions for conservation laws.&lt;/b&gt;&lt;br /&gt;&lt;i&gt;&lt;a href="http://groups.google.com/group/ioantlp/web/ImpNoLinEulr.pdf?hl=en"&gt;DG Implicit schemes for nonlinear Euler equations &lt;/a&gt;&lt;br /&gt;&lt;p&gt; &lt;a href="http://groups.google.com/group/ioantlp/web/2D_MHD.pdf?hl=en"&gt;DG numerical solutions for MHD equations&lt;/a&gt;&lt;/i&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7735848022985100293-5282054784563635973?l=toulio.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/5282054784563635973/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://toulio.blogspot.com/2009/06/my-papers.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/5282054784563635973'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/5282054784563635973'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/2009/06/my-papers.html' title='My Papers'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-7735848022985100293.post-4782270422952408967</id><published>2009-12-03T09:46:00.000-08:00</published><updated>2009-12-07T07:12:00.318-08:00</updated><category scheme='http://www.blogger.com/atom/ns#' term='September Sunday at the village'/><title type='text'>MyPhotos</title><content type='html'>&lt;SPAN class=fullpost&gt;&lt;p&gt;&lt;span class="fullpost"&gt;&lt;br /&gt;Photos from my village Chorigos&lt;br /&gt;&lt;P&gt;&lt;A href="http://3.bp.blogspot.com/_paT6dlY5x_g/SkYiRTVRCuI/AAAAAAAAADg/cXCl-YwRfKU/s1600-h/Ch_f7.jpg"&gt;&lt;IMG id=BLOGGER_PHOTO_ID_5352002887819004642 style="WIDTH: 320px; CURSOR: hand; HEIGHT: 240px" alt="" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SkYiRTVRCuI/AAAAAAAAADg/cXCl-YwRfKU/s320/Ch_f7.jpg" border=0&gt;&lt;/A&gt; &lt;A href="http://2.bp.blogspot.com/_paT6dlY5x_g/SkYiBdn8KKI/AAAAAAAAADY/09Lnjzl_lqg/s1600-h/Ch_f6.jpg"&gt;&lt;IMG id=BLOGGER_PHOTO_ID_5352002615703775394 style="WIDTH: 320px; CURSOR: hand; HEIGHT: 240px" alt="" src="http://2.bp.blogspot.com/_paT6dlY5x_g/SkYiBdn8KKI/AAAAAAAAADY/09Lnjzl_lqg/s320/Ch_f6.jpg" border=0&gt;&lt;/A&gt; &lt;A href="http://2.bp.blogspot.com/_paT6dlY5x_g/SkYdV70iS-I/AAAAAAAAADQ/ofzOKYhvqUg/s1600-h/Ch_f5.jpg"&gt;&lt;IMG id=BLOGGER_PHOTO_ID_5351997469848914914 style="WIDTH: 320px; CURSOR: hand; HEIGHT: 240px" alt="" src="http://2.bp.blogspot.com/_paT6dlY5x_g/SkYdV70iS-I/AAAAAAAAADQ/ofzOKYhvqUg/s320/Ch_f5.jpg" border=0&gt;&lt;/A&gt; &lt;A href="http://4.bp.blogspot.com/_paT6dlY5x_g/SkYdRC4Px5I/AAAAAAAAADI/qBdmWY3cu7I/s1600-h/Ch_f4.jpg"&gt;&lt;IMG id=BLOGGER_PHOTO_ID_5351997385844180882 style="WIDTH: 320px; CURSOR: hand; HEIGHT: 240px" alt="" src="http://4.bp.blogspot.com/_paT6dlY5x_g/SkYdRC4Px5I/AAAAAAAAADI/qBdmWY3cu7I/s320/Ch_f4.jpg" border=0&gt;&lt;/A&gt; &lt;A href="http://4.bp.blogspot.com/_paT6dlY5x_g/SkYdLbVeVxI/AAAAAAAAADA/ifi0viUQ_tA/s1600-h/Ch_f3.jpg"&gt;&lt;IMG id=BLOGGER_PHOTO_ID_5351997289330005778 style="WIDTH: 320px; CURSOR: hand; HEIGHT: 240px" alt="" src="http://4.bp.blogspot.com/_paT6dlY5x_g/SkYdLbVeVxI/AAAAAAAAADA/ifi0viUQ_tA/s320/Ch_f3.jpg" border=0&gt;&lt;/A&gt; &lt;A href="http://1.bp.blogspot.com/_paT6dlY5x_g/SkYdEl5-eRI/AAAAAAAAAC4/ihigKMwRtNA/s1600-h/Ch_f2.jpg"&gt;&lt;IMG id=BLOGGER_PHOTO_ID_5351997171908376850 style="WIDTH: 320px; CURSOR: hand; HEIGHT: 240px" alt="" src="http://1.bp.blogspot.com/_paT6dlY5x_g/SkYdEl5-eRI/AAAAAAAAAC4/ihigKMwRtNA/s320/Ch_f2.jpg" border=0&gt;&lt;/A&gt; &lt;A href="http://2.bp.blogspot.com/_paT6dlY5x_g/SkYc9qFTgJI/AAAAAAAAACw/NcGGTE_5Ebs/s1600-h/Ch_f1.jpg"&gt;&lt;IMG id=BLOGGER_PHOTO_ID_5351997052770549906 style="WIDTH: 320px; CURSOR: hand; HEIGHT: 240px" alt="" src="http://2.bp.blogspot.com/_paT6dlY5x_g/SkYc9qFTgJI/AAAAAAAAACw/NcGGTE_5Ebs/s320/Ch_f1.jpg" border=0&gt;&lt;/A&gt; &lt;A onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ7lVv5qMI/AAAAAAAAACQ/y-jbBgVGHTg/s1600-h/Chorigos.bmp"&gt;&lt;IMG id=BLOGGER_PHOTO_ID_5347597488972474562 style="FLOAT: left; MARGIN: 0px 10px 10px 0px; WIDTH: 320px; CURSOR: hand; HEIGHT: 240px" alt="" src="http://3.bp.blogspot.com/_paT6dlY5x_g/SjZ7lVv5qMI/AAAAAAAAACQ/y-jbBgVGHTg/s320/Chorigos.bmp" border=0&gt;&lt;/A&gt; &lt;A onblur="try {parent.deselectBloggerImageGracefully();} catch(e) {}" href="http://2.bp.blogspot.com/_paT6dlY5x_g/SjZ7-pQX7jI/AAAAAAAAACY/RVB3nAXtVD0/s1600-h/ZooPigi.bmp"&gt;&lt;IMG id=BLOGGER_PHOTO_ID_5347597923705679410 style="FLOAT: left; MARGIN: 0px 10px 10px 0px; WIDTH: 320px; CURSOR: hand; HEIGHT: 240px" alt="" src="http://2.bp.blogspot.com/_paT6dlY5x_g/SjZ7-pQX7jI/AAAAAAAAACY/RVB3nAXtVD0/s320/ZooPigi.bmp" border=0&gt;&lt;/A&gt; &lt;/SPAN&gt;&lt;br /&gt;&lt;object width="320" height="266" class="BLOG_video_class" id="BLOG_video-a0414e76b62bc49" classid="clsid:D27CDB6E-AE6D-11cf-96B8-444553540000" codebase="http://download.macromedia.com/pub/shockwave/cabs/flash/swflash.cab#version=6,0,40,0"&gt;&lt;param name="movie" value="http://www.youtube.com/get_player"&gt;&lt;param name="bgcolor" value="#FFFFFF"&gt;&lt;param name="allowfullscreen" value="true"&gt;&lt;param name="flashvars" value="flvurl=http://v4.nonxt3.googlevideo.com/videoplayback?id%3D0a0414e76b62bc49%26itag%3D5%26app%3Dblogger%26ip%3D0.0.0.0%26ipbits%3D0%26expire%3D1331666302%26sparams%3Did,itag,ip,ipbits,expire%26signature%3D831CBC187C14CD9FC3C64478805F94E8E9CF8C41.627608AEA2A03D9345EEF4B1A728279B2D023623%26key%3Dck1&amp;amp;iurl=http://video.google.com/ThumbnailServer2?app%3Dblogger%26contentid%3Da0414e76b62bc49%26offsetms%3D5000%26itag%3Dw160%26sigh%3D0qTeGFlc0J4Fp8fvHLwIYST5AL0&amp;amp;autoplay=0&amp;amp;ps=blogger"&gt;&lt;embed src="http://www.youtube.com/get_player" type="application/x-shockwave-flash"width="320" height="266" bgcolor="#FFFFFF"flashvars="flvurl=http://v4.nonxt3.googlevideo.com/videoplayback?id%3D0a0414e76b62bc49%26itag%3D5%26app%3Dblogger%26ip%3D0.0.0.0%26ipbits%3D0%26expire%3D1331666302%26sparams%3Did,itag,ip,ipbits,expire%26signature%3D831CBC187C14CD9FC3C64478805F94E8E9CF8C41.627608AEA2A03D9345EEF4B1A728279B2D023623%26key%3Dck1&amp;iurl=http://video.google.com/ThumbnailServer2?app%3Dblogger%26contentid%3Da0414e76b62bc49%26offsetms%3D5000%26itag%3Dw160%26sigh%3D0qTeGFlc0J4Fp8fvHLwIYST5AL0&amp;autoplay=0&amp;ps=blogger"allowFullScreen="true" /&gt;&lt;/object&gt;&lt;/P&gt;&lt;br /&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/7735848022985100293-4782270422952408967?l=toulio.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='enclosure' type='video/mp4' href='http://www.blogger.com/video-play.mp4?contentId=a0414e76b62bc49&amp;type=video%2Fmp4' length='0'/><link rel='replies' type='application/atom+xml' href='http://toulio.blogspot.com/feeds/4782270422952408967/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://toulio.blogspot.com/2009/06/myphotos.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/4782270422952408967'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/7735848022985100293/posts/default/4782270422952408967'/><link rel='alternate' type='text/html' href='http://toulio.blogspot.com/2009/06/myphotos.html' title='MyPhotos'/><author><name>toulio</name><uri>http://www.blogger.com/profile/00997611667222094536</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><media:thumbnail xmlns:media='http://search.yahoo.com/mrss/' url='http://3.bp.blogspot.com/_paT6dlY5x_g/SkYiRTVRCuI/AAAAAAAAADg/cXCl-YwRfKU/s72-c/Ch_f7.jpg' height='72' width='72'/><thr:total>0</thr:total></entry></feed>
