{"id":1155,"date":"2023-02-06T15:46:44","date_gmt":"2023-02-06T14:46:44","guid":{"rendered":"https:\/\/au.feri.um.si\/leoss\/?p=1155"},"modified":"2023-02-06T15:46:44","modified_gmt":"2023-02-06T14:46:44","slug":"miniature-fiber-optic-pitot-tube-sensor","status":"publish","type":"post","link":"https:\/\/au.jovo.cc\/leoss\/2023\/02\/06\/miniature-fiber-optic-pitot-tube-sensor\/","title":{"rendered":"Miniature fiber-optic Pitot tube sensor"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\">This paper presents a miniature fiber-optic Pitot tube for gas flow rate measurements created at the tip of an optical fiber. The proposed all-fiber sensor employs two in-fiber Fabry-Perot cavities\/chambers. The first chamber is arranged as a differential pressure sensor using a thin flexible silica diaphragm and two side holes for measurement of the difference between stagnation and static pressure, while the second chamber acts as a reference sensor for compensation of changes in the gas refractive index. The entire sensor is fusion-spliced, and is made out of sections of silica fibers and silica capillaries. It is appropriate for mid to high-velocity microfluidic gas flow sensing where miniature size is essential. Sensor operation is demonstrated in a flow velocity range between 0 to 260 m\/s with a resolution better than 1.5 m\/s. The sensor has a diameter of only 200 \u03bcm.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Published in: <\/strong><a href=\"https:\/\/ieeexplore.ieee.org\/xpl\/RecentIssue.jsp?punumber=7361\">IEEE Sensors Journal<\/a> ( Volume: 20, <a href=\"https:\/\/ieeexplore.ieee.org\/xpl\/tocresult.jsp?isnumber=9056594&amp;punumber=7361\">Issue: 9<\/a>, 01 May 2020) <\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>DOI: <\/strong><a rel=\"noreferrer noopener\" href=\"https:\/\/doi.org\/10.1109\/JSEN.2020.2966621\" target=\"_blank\">10.1109\/JSEN.2020.2966621<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>This paper presents a miniature fiber-optic Pitot tube for gas flow rate measurements created at the tip of an optical fiber. The proposed all-fiber sensor employs two in-fiber Fabry-Perot cavities\/chambers. The first chamber is arranged as a differential pressure sensor using a thin flexible silica diaphragm and two side holes for measurement of the difference [&hellip;]<\/p>\n","protected":false},"author":0,"featured_media":1013,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[30,31,10,13,15,5,25],"tags":[],"class_list":["post-1155","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-lomni-kolicnik","category-opticna-vlakna","category-mikro-obdelava","category-opticni-vlakenski-senzorji","category-ostali-opticni-vlakenski-senzorji","category-raziskovalno-delo","category-pressure-sensor"],"_links":{"self":[{"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/posts\/1155","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=1155"}],"version-history":[{"count":0,"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/posts\/1155\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/media\/1013"}],"wp:attachment":[{"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/media?parent=1155"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/categories?post=1155"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/au.jovo.cc\/leoss\/wp-json\/wp\/v2\/tags?post=1155"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}