{"id":92836,"date":"2018-03-11T10:11:59","date_gmt":"2018-03-11T10:11:59","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/redundancy-of-the-lhc-machine-protection-systems-in-case-of-magnet-failures\/"},"modified":"2018-03-11T10:11:59","modified_gmt":"2018-03-11T10:11:59","slug":"redundancy-of-the-lhc-machine-protection-systems-in-case-of-magnet-failures","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/simulacion\/redundancy-of-the-lhc-machine-protection-systems-in-case-of-magnet-failures\/","title":{"rendered":"Redundancy of the lhc machine protection systems in case of magnet failures"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Andr\u00e9s G\u00f3mez Alonso <\/strong><\/h2>\n<p>The\u00c2\u00a0large\u00c2\u00a0hadron\u00c2\u00a0collider\u00c2\u00a0(lhc)\u00c2\u00a0built\u00c2\u00a0at\u00c2\u00a0cern,\u00c2\u00a0the\u00c2\u00a0european\u00c2\u00a0laboratory\u00c2\u00a0for\u00c2\u00a0particle\u00c2\u00a0physics\u00c2\u00a0will\u00c2\u00a0accelerate\u00c2\u00a0high\u00c2\u00a0 intensity\u00c2\u00a0proton\u00c2\u00a0beams\u00c2\u00a0up\u00c2\u00a0to\u00c2\u00a0an\u00c2\u00a0energy\u00c2\u00a0of\u00c2\u00a07\u00c2\u00a0tev\u00c2\u00a0per\u00c2\u00a0proton.\u00c2\u00a0the\u00c2\u00a0energy\u00c2\u00a0stored\u00c2\u00a0in\u00c2\u00a0the\u00c2\u00a0lhc\u00c2\u00a0magnets\u00c2\u00a0reaches\u00c2\u00a0about\u00c2\u00a0 10ugj\u00c2\u00a0and\u00c2\u00a0each\u00c2\u00a0of \u00c2\u00a0 the\u00c2\u00a0proton\u00c2\u00a0beams\u00c2\u00a0stores\u00c2\u00a0about\u00c2\u00a0360\u00c2\u00a0mj\u00c2\u00a0at \u00c2\u00a0nominal\u00c2\u00a0collision\u00c2\u00a0energy.\u00c2\u00a0accidental \u00c2\u00a0release\u00c2\u00a0of \u00c2\u00a0 this\u00c2\u00a0 energy\u00c2\u00a0 in\u00c2\u00a0an\u00c2\u00a0uncontrolled\u00c2\u00a0way\u00c2\u00a0would\u00c2\u00a0 lead\u00c2\u00a0 to\u00c2\u00a0serious\u00c2\u00a0damage\u00c2\u00a0of \u00c2\u00a0 the\u00c2\u00a0accelerator \u00c2\u00a0equipment. \u00c2\u00a0the\u00c2\u00a0lhc\u00c2\u00a0machine\u00c2\u00a0 protection\u00c2\u00a0systems\u00c2\u00a0are\u00c2\u00a0designed\u00c2\u00a0to\u00c2\u00a0protect\u00c2\u00a0the\u00c2\u00a0accelerator\u00c2\u00a0against\u00c2\u00a0such\u00c2\u00a0uncontrolled\u00c2\u00a0release\u00c2\u00a0of\u00c2\u00a0the\u00c2\u00a0stored\u00c2\u00a0energy.\u00c2\u00a0 they\u00c2\u00a0provide\u00c2\u00a0constant\u00c2\u00a0monitoring\u00c2\u00a0of\u00c2\u00a0critical\u00c2\u00a0equipment,\u00c2\u00a0constant\u00c2\u00a0monitoring\u00c2\u00a0of\u00c2\u00a0the\u00c2\u00a0beam\u00c2\u00a0position\u00c2\u00a0and\u00c2\u00a0losses,\u00c2\u00a0a\u00c2\u00a0very\u00c2\u00a0 reliable\u00c2\u00a0beam\u00c2\u00a0dump\u00c2\u00a0system\u00c2\u00a0and\u00c2\u00a0 fast, \u00c2\u00a0very\u00c2\u00a0 reliable\u00c2\u00a0 interlock\u00c2\u00a0systems\u00c2\u00a0 to\u00c2\u00a0 transmit \u00c2\u00a0protection\u00c2\u00a0critical \u00c2\u00a0signals. \u00c2\u00a0while\u00c2\u00a0 protecting\u00c2\u00a0the\u00c2\u00a0accelerator\u00c2\u00a0in\u00c2\u00a0case\u00c2\u00a0of\u00c2\u00a0failure,\u00c2\u00a0the\u00c2\u00a0machine\u00c2\u00a0protection\u00c2\u00a0systems\u00c2\u00a0must\u00c2\u00a0also\u00c2\u00a0ensure\u00c2\u00a0maximum\u00c2\u00a0operational\u00c2\u00a0 availability\u00c2\u00a0of\u00c2\u00a0the\u00c2\u00a0lhc\u00c2\u00a0beams. magnet \u00c2\u00a0 failures\u00c2\u00a0produce\u00c2\u00a0 the\u00c2\u00a0 fastest \u00c2\u00a0effects\u00c2\u00a0on\u00c2\u00a0 the\u00c2\u00a0beam\u00c2\u00a0and\u00c2\u00a0are\u00c2\u00a0most \u00c2\u00a0critical \u00c2\u00a0with\u00c2\u00a0respect \u00c2\u00a0 to\u00c2\u00a0machine\u00c2\u00a0protection.\u00c2\u00a0 quenches\u00c2\u00a0 (loss\u00c2\u00a0of \u00c2\u00a0magnet \u00c2\u00a0superconductivity) \u00c2\u00a0and\u00c2\u00a0 failures\u00c2\u00a0of \u00c2\u00a0 the\u00c2\u00a0power \u00c2\u00a0converters\u00c2\u00a0 (powering\u00c2\u00a0 failures) \u00c2\u00a0have\u00c2\u00a0been\u00c2\u00a0 considered.\u00c2\u00a0these\u00c2\u00a0failures\u00c2\u00a0produce\u00c2\u00a0a\u00c2\u00a0current\u00c2\u00a0decay\u00c2\u00a0in\u00c2\u00a0the\u00c2\u00a0magnet\u00c2\u00a0and\u00c2\u00a0the\u00c2\u00a0corresponding\u00c2\u00a0decay\u00c2\u00a0in\u00c2\u00a0the\u00c2\u00a0magnetic\u00c2\u00a0field.\u00c2\u00a0 the\u00c2\u00a0current\u00c2\u00a0decay\u00c2\u00a0after\u00c2\u00a0a\u00c2\u00a0quench\u00c2\u00a0has\u00c2\u00a0been\u00c2\u00a0modeled\u00c2\u00a0by\u00c2\u00a0a\u00c2\u00a0gaussian\u00c2\u00a0curve\u00c2\u00a0based\u00c2\u00a0on\u00c2\u00a0previous\u00c2\u00a0studies.\u00c2\u00a0the\u00c2\u00a0current\u00c2\u00a0 decay\u00c2\u00a0generated\u00c2\u00a0by\u00c2\u00a0powering\u00c2\u00a0failures\u00c2\u00a0has\u00c2\u00a0been\u00c2\u00a0considered\u00c2\u00a0exponential. in\u00c2\u00a0order\u00c2\u00a0to\u00c2\u00a0evaluate\u00c2\u00a0the\u00c2\u00a0effects\u00c2\u00a0of\u00c2\u00a0magnet\u00c2\u00a0failures\u00c2\u00a0on\u00c2\u00a0the\u00c2\u00a0beam,\u00c2\u00a0particle\u00c2\u00a0tracking\u00c2\u00a0with\u00c2\u00a0variable\u00c2\u00a0magnetic\u00c2\u00a0fields\u00c2\u00a0has\u00c2\u00a0been\u00c2\u00a0 done\u00c2\u00a0using\u00c2\u00a0 the\u00c2\u00a0madx\u00c2\u00a0program. \u00c2\u00a0dipole\u00c2\u00a0 failures\u00c2\u00a0produce\u00c2\u00a0a\u00c2\u00a0closed\u00c2\u00a0orbit \u00c2\u00a0distortion\u00c2\u00a0 that \u00c2\u00a0can\u00c2\u00a0be\u00c2\u00a0easily\u00c2\u00a0determined\u00c2\u00a0 analytically.\u00c2\u00a0losses\u00c2\u00a0produced\u00c2\u00a0by\u00c2\u00a0dipole\u00c2\u00a0failures\u00c2\u00a0are\u00c2\u00a0generally\u00c2\u00a0localized.\u00c2\u00a0quadrupole\u00c2\u00a0failures\u00c2\u00a0lead\u00c2\u00a0to\u00c2\u00a0beta\u00c2\u00a0beating\u00c2\u00a0and\u00c2\u00a0 tune\u00c2\u00a0shift,\u00c2\u00a0which\u00c2\u00a0in\u00c2\u00a0the\u00c2\u00a0transverse\u00c2\u00a0plane translate\u00c2\u00a0into\u00c2\u00a0either\u00c2\u00a0defocusing\u00c2\u00a0or\u00c2\u00a0displacement\u00c2\u00a0of\u00c2\u00a0the\u00c2\u00a0beam.\u00c2\u00a0the\u00c2\u00a0crossing\u00c2\u00a0of\u00c2\u00a0non\u00c2\u00adlinear\u00c2\u00a0resonances\u00c2\u00a0induced\u00c2\u00a0by\u00c2\u00a0the\u00c2\u00a0 tune\u00c2\u00a0shift\u00c2\u00a0can\u00c2\u00a0generate\u00c2\u00a0losses\u00c2\u00a0of\u00c2\u00a0up\u00c2\u00a0to\u00c2\u00a010%\u00c2\u00a0of\u00c2\u00a0the\u00c2\u00a0beam\u00c2\u00a0intensity,\u00c2\u00a0and\u00c2\u00a0beam\u00c2\u00a0losses\u00c2\u00a0induced\u00c2\u00a0by\u00c2\u00a0quadrupole\u00c2\u00a0failures\u00c2\u00a0 may\u00c2\u00a0be\u00c2\u00a0distributed\u00c2\u00a0over\u00c2\u00a0many\u00c2\u00a0locations. the\u00c2\u00a0 transverse\u00c2\u00a0distribution\u00c2\u00a0of \u00c2\u00a0 the\u00c2\u00a0primary\u00c2\u00a0 losses\u00c2\u00a0at \u00c2\u00a0 the\u00c2\u00a0collimators\u00c2\u00a0can\u00c2\u00a0be\u00c2\u00a0described\u00c2\u00a0by\u00c2\u00a0a\u00c2\u00a0 function\u00c2\u00a0of \u00c2\u00a0exponential\u00c2\u00a0 nature, \u00c2\u00a0allowing\u00c2\u00a0a\u00c2\u00a0 fast \u00c2\u00a0characterization\u00c2\u00a0of \u00c2\u00a0 the\u00c2\u00a0 impact \u00c2\u00a0 from\u00c2\u00a0 the\u00c2\u00a0parameters\u00c2\u00a0of \u00c2\u00a0 the\u00c2\u00a0 function. \u00c2\u00a0dipole\u00c2\u00a0and\u00c2\u00a0quadrupole\u00c2\u00a0 failures\u00c2\u00a0lead\u00c2\u00a0to\u00c2\u00a0primary\u00c2\u00a0impacts\u00c2\u00a0that\u00c2\u00a0are\u00c2\u00a0not\u00c2\u00a0significantly\u00c2\u00a0different\u00c2\u00a0in\u00c2\u00a0shape\u00c2\u00a0or\u00c2\u00a0size,\u00c2\u00a0and\u00c2\u00a0in\u00c2\u00a0both\u00c2\u00a0cases\u00c2\u00a0faster\u00c2\u00a0failures\u00c2\u00a0 produce\u00c2\u00a0broader\u00c2\u00a0impacts.\u00c2\u00a0the\u00c2\u00a0average\u00c2\u00a0impact\u00c2\u00a0parameter\u00c2\u00a0for\u00c2\u00a0the\u00c2\u00a0cases\u00c2\u00a0studied\u00c2\u00a0ranges\u00c2\u00a0from\u00c2\u00a0less\u00c2\u00a0than\u00c2\u00a05\u00c2\u00a0\u00c2\u00bfm\u00c2\u00a0to\u00c2\u00a0about\u00c2\u00a0 1umm.\u00c2\u00a0the\u00c2\u00a0amount\u00c2\u00a0of\u00c2\u00a0losses\u00c2\u00a0reaching\u00c2\u00a0the\u00c2\u00a0superconducting\u00c2\u00a0elements\u00c2\u00a0from\u00c2\u00a0particles\u00c2\u00a0scattered\u00c2\u00a0after\u00c2\u00a0a\u00c2\u00a0primary\u00c2\u00a0impact\u00c2\u00a0is\u00c2\u00a0 greater\u00c2\u00a0for\u00c2\u00a0impacts\u00c2\u00a0at\u00c2\u00a0collimators\u00c2\u00a0outside\u00c2\u00a0or\u00c2\u00a0at\u00c2\u00a0the\u00c2\u00a0end\u00c2\u00a0of\u00c2\u00a0the\u00c2\u00a0cleaning\u00c2\u00a0insertions.\u00c2\u00a0it\u00c2\u00a0may\u00c2\u00a0reach\u00c2\u00a0up\u00c2\u00a0to\u00c2\u00a010%\u00c2\u00a0of\u00c2\u00a0the\u00c2\u00a0beam\u00c2\u00a0 intensity\u00c2\u00a0at \u00c2\u00a0450\u00c2\u00a0gev\u00c2\u00a0and\u00c2\u00a01%\u00c2\u00a0at \u00c2\u00a07\u00c2\u00a0tev\u00c2\u00a0and\u00c2\u00a0 in\u00c2\u00a0most \u00c2\u00a0cases, \u00c2\u00a0 it \u00c2\u00a0decreases\u00c2\u00a0with\u00c2\u00a0 increasing\u00c2\u00a0 impact \u00c2\u00a0parameter \u00c2\u00a0of \u00c2\u00a0 the\u00c2\u00a0 primary\u00c2\u00a0impact.\u00c2\u00a0 with\u00c2\u00a0circulating\u00c2\u00a0beam\u00c2\u00a0at\u00c2\u00a0lhc,\u00c2\u00a0powering\u00c2\u00a0failures\u00c2\u00a0of\u00c2\u00a0the\u00c2\u00a0d1\u00c2\u00a0dipoles\u00c2\u00a0at\u00c2\u00a0ir1\u00c2\u00a0and\u00c2\u00a0ir5\u00c2\u00a0produce\u00c2\u00a0the\u00c2\u00a0fastest\u00c2\u00a0losses\u00c2\u00a0both\u00c2\u00a0at\u00c2\u00a0 450\u00c2\u00a0gev\u00c2\u00a0and\u00c2\u00a07\u00c2\u00a0tev,\u00c2\u00a0reaching\u00c2\u00a0the\u00c2\u00a0damage\u00c2\u00a0level\u00c2\u00a0in\u00c2\u00a0less\u00c2\u00a0than\u00c2\u00a03\u00c2\u00a0ms\u00c2\u00a0in\u00c2\u00a0both\u00c2\u00a0cases.\u00c2\u00a0other\u00c2\u00a0failures\u00c2\u00a0of\u00c2\u00a0normal\u00c2\u00a0conducting\u00c2\u00a0 magnets\u00c2\u00a0could\u00c2\u00a0produce\u00c2\u00a0damage\u00c2\u00a0after\u00c2\u00a0about\u00c2\u00a010\u00c2\u00a0ms\u00c2\u00a0and\u00c2\u00a0quenches\u00c2\u00a0in\u00c2\u00a0the\u00c2\u00a0main\u00c2\u00a0superconducting\u00c2\u00a0dipoles\u00c2\u00a0may\u00c2\u00a0lead\u00c2\u00a0to\u00c2\u00a0 damage\u00c2\u00a0about\u00c2\u00a015\u00c2\u00a0ms\u00c2\u00a0after\u00c2\u00a0the\u00c2\u00a0current\u00c2\u00a0decay\u00c2\u00a0starts.\u00c2\u00a0redundancy\u00c2\u00a0is\u00c2\u00a0ensured\u00c2\u00a0when,\u00c2\u00a0for\u00c2\u00a0a\u00c2\u00a0given\u00c2\u00a0failure,\u00c2\u00a0at\u00c2\u00a0least\u00c2\u00a0two\u00c2\u00a0 independent\u00c2\u00a0protection\u00c2\u00a0systems\u00c2\u00a0react\u00c2\u00a0on\u00c2\u00a0time.\u00c2\u00a0the\u00c2\u00a0beam\u00c2\u00a0loss\u00c2\u00a0monitors\u00c2\u00a0are\u00c2\u00a0able\u00c2\u00a0to\u00c2\u00a0request\u00c2\u00a0a\u00c2\u00a0beam\u00c2\u00a0dump\u00c2\u00a0in\u00c2\u00a0time\u00c2\u00a0for\u00c2\u00a0 every\u00c2\u00a0failure\u00c2\u00a0case\u00c2\u00a0considered.\u00c2\u00a0in\u00c2\u00a0combination\u00c2\u00a0with\u00c2\u00a0the\u00c2\u00a0quench\u00c2\u00a0protection\u00c2\u00a0system,\u00c2\u00a0the\u00c2\u00a0powering\u00c2\u00a0interlock\u00c2\u00a0controller\u00c2\u00a0 and\u00c2\u00a0the\u00c2\u00a0fast\u00c2\u00a0magnet\u00c2\u00a0current\u00c2\u00a0change\u00c2\u00a0monitors\u00c2\u00a0most\u00c2\u00a0failure\u00c2\u00a0cases\u00c2\u00a0are\u00c2\u00a0redundantly\u00c2\u00a0protected.\u00c2\u00a0only\u00c2\u00a0quenches\u00c2\u00a0of\u00c2\u00a0some\u00c2\u00a0 superconducting\u00c2\u00a0dipoles\u00c2\u00a0are\u00c2\u00a0not \u00c2\u00a0 redundantly\u00c2\u00a0protected\u00c2\u00a0with\u00c2\u00a0 these\u00c2\u00a0 systems, \u00c2\u00a0but \u00c2\u00a0 redundancy\u00c2\u00a0can\u00c2\u00a0be\u00c2\u00a0ensured\u00c2\u00a0by\u00c2\u00a0 additional\u00c2\u00a0systems,\u00c2\u00a0such\u00c2\u00a0as\u00c2\u00a0a\u00c2\u00a0fast\u00c2\u00a0beam\u00c2\u00a0current\u00c2\u00a0monitor.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Redundancy of the lhc machine protection systems in case of magnet failures<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Redundancy of the lhc machine protection systems in case of magnet failures <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Andr\u00e9s G\u00f3mez Alonso <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Polit\u00e9cnica de catalunya<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 17\/04\/2009<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n<h3>Direcci\u00f3n y tribunal<\/h3>\n<ul>\n<li><strong>Director de la tesis<\/strong>\n<ul>\n<li>Francisco Calvi\u00f1o Tavares<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Luis Garc\u00eda tabares <\/li>\n<li>mathias Vogt (vocal)<\/li>\n<li>bernhard Holzer (vocal)<\/li>\n<li>Antonio Vergara fern\u00e1ndez (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Andr\u00e9s G\u00f3mez Alonso The\u00c2\u00a0large\u00c2\u00a0hadron\u00c2\u00a0collider\u00c2\u00a0(lhc)\u00c2\u00a0built\u00c2\u00a0at\u00c2\u00a0cern,\u00c2\u00a0the\u00c2\u00a0european\u00c2\u00a0laboratory\u00c2\u00a0for\u00c2\u00a0particle\u00c2\u00a0physics\u00c2\u00a0will\u00c2\u00a0accelerate\u00c2\u00a0high\u00c2\u00a0 intensity\u00c2\u00a0proton\u00c2\u00a0beams\u00c2\u00a0up\u00c2\u00a0to\u00c2\u00a0an\u00c2\u00a0energy\u00c2\u00a0of\u00c2\u00a07\u00c2\u00a0tev\u00c2\u00a0per\u00c2\u00a0proton.\u00c2\u00a0the\u00c2\u00a0energy\u00c2\u00a0stored\u00c2\u00a0in\u00c2\u00a0the\u00c2\u00a0lhc\u00c2\u00a0magnets\u00c2\u00a0reaches\u00c2\u00a0about\u00c2\u00a0 10ugj\u00c2\u00a0and\u00c2\u00a0each\u00c2\u00a0of \u00c2\u00a0 the\u00c2\u00a0proton\u00c2\u00a0beams\u00c2\u00a0stores\u00c2\u00a0about\u00c2\u00a0360\u00c2\u00a0mj\u00c2\u00a0at \u00c2\u00a0nominal\u00c2\u00a0collision\u00c2\u00a0energy.\u00c2\u00a0accidental \u00c2\u00a0release\u00c2\u00a0of \u00c2\u00a0 this\u00c2\u00a0 energy\u00c2\u00a0 in\u00c2\u00a0an\u00c2\u00a0uncontrolled\u00c2\u00a0way\u00c2\u00a0would\u00c2\u00a0 lead\u00c2\u00a0 to\u00c2\u00a0serious\u00c2\u00a0damage\u00c2\u00a0of \u00c2\u00a0 [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"site-sidebar-layout":"default","site-content-layout":"","ast-site-content-layout":"","site-content-style":"default","site-sidebar-style":"default","ast-global-header-display":"","ast-banner-title-visibility":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","theme-transparent-header-meta":"","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","astra-migrate-meta-layouts":"default","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"background-color":"var(--ast-global-color-4)","background-image":"","background-repeat":"repeat","background-position":"center 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