Fiber Bragg gratings as transient thermal gradient sensors
We experimentally subject a fiber Bragg grating to an unknown, variable temperature gradient. We use the full-spectral response of the grating to determine the magnitude of the gradient over the length of the grating via the full width at quarter maximum bandwidth. The experimental bandwidth and spe...
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| Published in | Optical engineering Vol. 55; no. 11; p. 114102 |
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| Main Authors | , , , , |
| Format | Journal Article |
| Language | English |
| Published |
Society of Photo-Optical Instrumentation Engineers
01.11.2016
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| Subjects | |
| Online Access | Get full text |
| ISSN | 0091-3286 1560-2303 |
| DOI | 10.1117/1.OE.55.11.114102 |
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| Abstract | We experimentally subject a fiber Bragg grating to an unknown, variable temperature gradient. We use the full-spectral response of the grating to determine the magnitude of the gradient over the length of the grating via the full width at quarter maximum bandwidth. The experimental bandwidth and spectrum deformation were compared with a numerical model consisting of an analytical heat transfer model, a finite element analysis model, and the transfer matrix (T-matrix) method. The numerical model showed excellent agreement with the experimental results when the T-matrix method was modified to include the slope of the gradient in addition to the magnitude of the gradient. |
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| AbstractList | We experimentally subject a fiber Bragg grating to an unknown, variable temperature gradient. We use the full-spectral response of the grating to determine the magnitude of the gradient over the length of the grating via the full width at quarter maximum bandwidth. The experimental bandwidth and spectrum deformation were compared with a numerical model consisting of an analytical heat transfer model, a finite element analysis model, and the transfer matrix (T-matrix) method. The numerical model showed excellent agreement with the experimental results when the T-matrix method was modified to include the slope of the gradient in addition to the magnitude of the gradient. |
| Author | Costa, Joannes M Hackney, Drew A Moslehi, Behzad Black, Richard J Peters, Kara J |
| Author_xml | – sequence: 1 givenname: Drew A surname: Hackney fullname: Hackney, Drew A organization: aNorth Carolina State University, Department of Mechanical and Aerospace Engineering, Campus Box 7910, Raleigh, North Carolina 27695, United States – sequence: 2 givenname: Kara J surname: Peters fullname: Peters, Kara J email: kjpeters@ncsu.edu organization: aNorth Carolina State University, Department of Mechanical and Aerospace Engineering, Campus Box 7910, Raleigh, North Carolina 27695, United States – sequence: 3 givenname: Richard J surname: Black fullname: Black, Richard J email: kjpeters@ncsu.edu organization: bIntelligent Fiber Optic Systems Corporation, 2363 Calle Del Mundo, Santa Clara, California 95054, United States – sequence: 4 givenname: Joannes M surname: Costa fullname: Costa, Joannes M organization: bIntelligent Fiber Optic Systems Corporation, 2363 Calle Del Mundo, Santa Clara, California 95054, United States – sequence: 5 givenname: Behzad surname: Moslehi fullname: Moslehi, Behzad organization: bIntelligent Fiber Optic Systems Corporation, 2363 Calle Del Mundo, Santa Clara, California 95054, United States |
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| Cites_doi | 10.1364/OL.19.002027 10.1063/1.124085 10.1117/12.2057942 10.1088/0964-1726/10/2/321 10.1177/1099636207064457 10.1109/68.769730 10.1117/12.862227 10.1117/1.1382642 10.1117/12.672853 10.1364/AO.26.003474 10.1177/1045389X11414220 10.1109/JLT.2004.833281 10.1016/S0266-3538(01)00037-9 |
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| Keywords | temperature gradient transfer matrix method fiber Bragg grating full spectrum |
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