{"id":856,"date":"2025-01-11T17:29:54","date_gmt":"2025-01-11T16:29:54","guid":{"rendered":"https:\/\/mastertechq.lpl.univ-paris13.fr\/?page_id=856"},"modified":"2025-01-20T19:33:09","modified_gmt":"2025-01-20T18:33:09","slug":"physique-pour-les-technologies-quantiques-2-2","status":"publish","type":"page","link":"https:\/\/mastertechq.lpl.univ-paris13.fr\/?page_id=856","title":{"rendered":"Physique pour les Technologies Quantiques 2-2"},"content":{"rendered":"\n<h2 class=\"wp-block-heading\">Physique pour les Technologies Quantiques 2<\/h2>\n\n\n\n<h3 class=\"wp-block-heading\"><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-palette-color-1-color\">Lignes, guides, fibres<\/mark><\/h3>\n\n\n\n<div id=\"wp-block-themeisle-blocks-advanced-columns-d885d8ee\" class=\"wp-block-themeisle-blocks-advanced-columns has-2-columns has-desktop-twoOne-layout has-tablet-equal-layout has-mobile-collapsedRows-layout has-vertical-unset\"><div class=\"wp-block-themeisle-blocks-advanced-columns-overlay\"><\/div><div class=\"innerblocks-wrap\">\n<div id=\"wp-block-themeisle-blocks-advanced-column-ec83570e\" class=\"wp-block-themeisle-blocks-advanced-column\">\n<h5 class=\"wp-block-heading\">Programme :<\/h5>\n\n\n\n<h6 class=\"wp-block-heading\">Introduction : <strong>Propagation libre et guid\u00e9e \u2013 Syst\u00e8mes de transmission<\/strong><\/h6>\n\n\n\n<p>Objectifs du cours.<br>Ondes \u00e9lectromagn\u00e9tiques.<br>Les diff\u00e9rents supports de transmission.<\/p>\n\n\n\n<h6 class=\"wp-block-heading\">I &#8211; Rappels sur les ondes \u00e9lectromagn\u00e9tiques<\/h6>\n\n\n\n<ol class=\"wp-block-list\">\n<li>Les \u00e9quations de Maxwell<\/li>\n\n\n\n<li>Propagation d\u2019ondes planes dans le vide<\/li>\n\n\n\n<li>Les diff\u00e9rents milieux m\u00e9talliques ou isolants<\/li>\n\n\n\n<li>Propagation dans un milieu di\u00e9lectrique parfait<\/li>\n\n\n\n<li>Propagation dans les milieux absorbants (ou avec pertes)<\/li>\n\n\n\n<li>Passage d\u2019un milieu \u00e0 un autre : r\u00e9flexion et r\u00e9fraction<\/li>\n<\/ol>\n\n\n\n<h6 class=\"wp-block-heading\">II &#8211; Les guides d\u2019ondes m\u00e9talliques<\/h6>\n\n\n\n<ol class=\"wp-block-list\">\n<li>Guidage par 2 plans conducteurs<\/li>\n\n\n\n<li>Guide \u00e0 section rectangulaire<\/li>\n\n\n\n<li>Pertes dans un guide m\u00e9tallique<\/li>\n\n\n\n<li>Cavit\u00e9s<\/li>\n<\/ol>\n\n\n\n<h6 class=\"wp-block-heading\">III &#8211; Les guides d\u2019ondes di\u00e9lectriques<\/h6>\n\n\n\n<ol class=\"wp-block-list\">\n<li>Les fibres optiques : approche g\u00e9om\u00e9trique<\/li>\n\n\n\n<li>Modes dans les fibres optiques<\/li>\n\n\n\n<li>Att\u00e9nuation, pertes dans les fibres optiques<\/li>\n\n\n\n<li>Modes de propagation : \u00e9tude \u00e9lectromagn\u00e9tique<\/li>\n\n\n\n<li>Dispersion dans une fibre optique<\/li>\n\n\n\n<li>Conclusion \u2013 Autres caract\u00e9ristiques des fibres optiques<\/li>\n<\/ol>\n\n\n\n<h6 class=\"wp-block-heading\">IV &#8211; Les lignes de transmission<\/h6>\n\n\n\n<ol class=\"wp-block-list\">\n<li>Mod\u00e9lisation d\u2019une ligne de transmission<\/li>\n\n\n\n<li>\u00c9quation des t\u00e9l\u00e9graphistes<\/li>\n\n\n\n<li>Adaptation d\u2019imp\u00e9dance<\/li>\n<\/ol>\n\n\n\n<div style=\"height:34px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<p><strong>Enseignant :<\/strong> <a href=\"https:\/\/mastertechq.lpl.univ-paris13.fr\/?page_id=1250\">Laurent Longchambon<\/a><\/p>\n<\/div>\n\n\n\n<div id=\"wp-block-themeisle-blocks-advanced-column-75b1f3ce\" class=\"wp-block-themeisle-blocks-advanced-column\">\n<div class=\"wp-block-group is-content-justification-center is-nowrap is-layout-flex wp-container-core-group-is-layout-23441af8 wp-block-group-is-layout-flex\">\n<div id=\"wp-block-themeisle-blocks-slider-4d728d3d\" class=\"wp-block-themeisle-blocks-slider alignwide glide\" data-per-view=\"1\" data-gap=\"0\" data-peek=\"0\" data-autoplay=\"4000\" data-height=\"400px\" data-hide-arrows=\"true\" data-transition=\"ease-in\"><div class=\"glide__track\" data-glide-el=\"track\"><div class=\"glide__slides\"><div class=\"wp-block-themeisle-blocks-slider-item-wrapper glide__slide\" tabindex=\"0\"><figure><img decoding=\"async\" class=\"wp-block-themeisle-blocks-slider-item\" src=\"https:\/\/mastertechq.lpl.univ-paris13.fr\/wp-content\/uploads\/2025\/01\/CNRS_20180037_0019-1024x1024.jpg\" alt=\"\" title=\"\" data-id=\"938\"\/><figcaption>Arriv\u00e9e de la fibre optique du SYRTE au LPL (43 km) <\/figcaption><\/figure><\/div><div class=\"wp-block-themeisle-blocks-slider-item-wrapper glide__slide\" tabindex=\"0\"><figure><img decoding=\"async\" class=\"wp-block-themeisle-blocks-slider-item\" src=\"https:\/\/mastertechq.lpl.univ-paris13.fr\/wp-content\/uploads\/2025\/01\/fibre-1024x768.jpg\" alt=\"\" title=\"\" data-id=\"936\"\/><\/figure><\/div><\/div><div class=\"glide__bullets\" data-glide-el=\"controls[nav]\"><button class=\"glide__bullet\" data-glide-dir=\"=0\"><\/button><button class=\"glide__bullet\" data-glide-dir=\"=1\"><\/button><\/div><\/div><\/div>\n<\/div>\n\n\n\n<div style=\"height:30px;width:0px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<figure class=\"wp-block-table aligncenter is-style-stripes\" style=\"font-style:normal;font-weight:400\"><table class=\"has-background has-fixed-layout\" style=\"background-color:#e7b5c3;border-width:2px\"><tbody><tr><td>CM<\/td><td>27 H<\/td><\/tr><tr><td>TD<\/td><td>18 H<\/td><\/tr><tr><td>TP<\/td><td>12 H<\/td><\/tr><tr><td>ECTS<\/td><td>5<\/td><\/tr><tr><td>Lieu<\/td><td>Villetaneuse<\/td><\/tr><tr><td>Langue<\/td><td>French<\/td><\/tr><\/tbody><\/table><\/figure>\n<\/div>\n<\/div><\/div>\n","protected":false},"excerpt":{"rendered":"<p>Physique pour les Technologies Quantiques 2 Lignes, guides, fibres<\/p>\n","protected":false},"author":2,"featured_media":0,"parent":302,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_themeisle_gutenberg_block_has_review":false,"footnotes":""},"class_list":["post-856","page","type-page","status-publish","hentry"],"blocksy_meta":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.2 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Physique pour les Technologies Quantiques 2-2 - Master TechQ<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/mastertechq.lpl.univ-paris13.fr\/?page_id=856\" \/>\n<meta property=\"og:locale\" content=\"fr_FR\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Physique pour les Technologies Quantiques 2-2 - Master TechQ\" \/>\n<meta property=\"og:description\" content=\"Physique pour les Technologies Quantiques 2 Lignes, guides, fibres\" \/>\n<meta property=\"og:url\" content=\"https:\/\/mastertechq.lpl.univ-paris13.fr\/?page_id=856\" \/>\n<meta property=\"og:site_name\" content=\"Master TechQ\" \/>\n<meta property=\"article:modified_time\" content=\"2025-01-20T18:33:09+00:00\" \/>\n<meta property=\"og:image\" content=\"https:\/\/mastertechq.lpl.univ-paris13.fr\/wp-content\/uploads\/2025\/01\/CNRS_20180037_0019-1024x1024.jpg\" \/>\n<meta name=\"twitter:card\" content=\"summary_large_image\" \/>\n<meta name=\"twitter:label1\" content=\"Dur\u00e9e de lecture estim\u00e9e\" \/>\n\t<meta name=\"twitter:data1\" content=\"2 minutes\" \/>\n<script type=\"application\/ld+json\" class=\"yoast-schema-graph\">{\"@context\":\"https:\/\/schema.org\",\"@graph\":[{\"@type\":\"WebPage\",\"@id\":\"https:\/\/mastertechq.lpl.univ-paris13.fr\/?page_id=856\",\"url\":\"https:\/\/mastertechq.lpl.univ-paris13.fr\/?page_id=856\",\"name\":\"Physique pour les Technologies Quantiques 2-2 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