{"id":384,"date":"2022-03-10T11:44:57","date_gmt":"2022-03-10T10:44:57","guid":{"rendered":"http:\/\/au.feri.um.si\/leoss\/?p=384"},"modified":"2022-03-10T11:44:57","modified_gmt":"2022-03-10T10:44:57","slug":"interrogation-of-fbgs-and-fbgs-arrays-using-standard-telecom-dfb-diode","status":"publish","type":"post","link":"https:\/\/au.jovo.cc\/leoss\/2022\/03\/10\/interrogation-of-fbgs-and-fbgs-arrays-using-standard-telecom-dfb-diode\/","title":{"rendered":"Interrogation of FBGs and FBGs arrays using standard telecom DFB diode"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\">An efficient fiber Bragg grating (FBG) sensor integration system, which utilizes a small number of standard Telecom opto-electronics components, is presented in this paper. Wavelength-swept optical pulses were generated by driving a standard telecom DFB laser diode by high amplitude (&gt;3 A) and short duration (300 ns) current pulses. A total laser diode&#8217;s wavelength sweep in excess of 10 nm was achieved, which allows for simultaneous interrogation of several FBGs within similar wavelengths. The application of short duration wavelength-swept optical pulses also allows for time division multiplexing of small FBG arrays containing FBGs with overlapping characteristic wavelengths. When a short, wavelength-swept optical pulse is launched into the fiber containing single or multiple FBGs along its length, fractions of the launched pulse are back-reflected towards the detector. Since the launched pulse wavelength changes over the time, the reflections from the FBGs occur in the time moments that depend on the FBGs&#8217; characteristic wavelengths. Measurement of the time delay among back-reflected optical pulses is then used to determine the FBGs characteristic wavelengths. The experimental system demonstrated FBG wavelength readout resolution, which exceeded 3 pm at 1 KHz sampling rate, maximum sampling rate of over 40 KHz, and capability to readout\/demultiplex over 30 FBGs located down a single optical fiber.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/ieeexplore.ieee.org\/document\/7589097\">https:\/\/ieeexplore.ieee.org\/document\/7589097<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>An efficient fiber Bragg grating (FBG) sensor integration system, which utilizes a small number of standard Telecom opto-electronics components, is presented in this paper. Wavelength-swept optical pulses were generated by driving a standard telecom DFB laser diode by high amplitude (&gt;3 A) and short duration (300 ns) current pulses. A total laser diode&#8217;s wavelength sweep [&hellip;]<\/p>\n","protected":false},"author":0,"featured_media":1242,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[14,5,19],"tags":[],"class_list":["post-384","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-opto-elektronski","category-raziskovalno-delo","category-signal-interrogators"],"_links":{"self":[{"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/posts\/384","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/types\/post"}],"replies":[{"embeddable":true,"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/comments?post=384"}],"version-history":[{"count":0,"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/posts\/384\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/media\/1242"}],"wp:attachment":[{"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/media?parent=384"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/categories?post=384"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/tags?post=384"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}