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| Naji, M. |
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| Motta, Antonella |
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| Aletan, Dirar |
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| Mohamed, Tarek |
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| Ertürk, Emre |
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| Taccardi, Nicola |
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| Kononenko, Denys |
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| Petrov, R. H. | Madrid |
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| Alshaaer, Mazen | Brussels |
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| Bih, L. |
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| Casati, R. |
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| Muller, Hermance |
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| Kočí, Jan | Prague |
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| Šuljagić, Marija |
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| Kalteremidou, Kalliopi-Artemi | Brussels |
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| Azam, Siraj |
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| Ospanova, Alyiya |
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| Blanpain, Bart |
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| Ali, M. A. |
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| Popa, V. |
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| Rančić, M. |
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| Ollier, Nadège |
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| Azevedo, Nuno Monteiro |
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| Landes, Michael |
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| Rignanese, Gian-Marco |
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Ferreira, Ms
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Topics
Publications (10/10 displayed)
- 2018Optical Fiber Tip Sensor for the Measurement of Glucose Aqueous Solutionscitations
- 2018Glucose measurements with optical fiber sensor based on coreless silica fiber
- 2018Determination of thermo-optic coefficient of ethanol-water mixtures with optical fiber tip sensorcitations
- 2017Fabry-Perot interferometer based on array of microspheres for temperature sensing
- 2014Post-processing fibers for sensing applications
- 2013Next generation of Fabry-Perot sensors for high-temperaturecitations
- 2013Microcavity Tip Temperature Sensor based on Post-Processing
- 2013Post-Processing of Fabry-Perot Microcavity Tip Sensorcitations
- 2012Towards the control of highly sensitive Fabry-Perot strain sensor based on hollow-core ring photonic crystal fibercitations
- 2011Simultaneous measurement of strain and temperature using fiber Bragg grating sensors embedded in hybrid composite laminatescitations
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article
Simultaneous measurement of strain and temperature using fiber Bragg grating sensors embedded in hybrid composite laminates
Abstract
The use of fiber Bragg grating sensors embedded in hybrid composite laminates for simultaneous measurement of strain and temperature is proposed. The hybrid structure, formed by a pre-impregnated thermoset and thermoplastic composites, contains one single fiber Bragg grating embedded in each material, connected in series with each other. A different response is observed when the smart composite laminate is subjected to strain and to temperature. This is expected due to the distinct properties presented by each material. The rms deviation obtained for a temperature range between 20 and 60 degrees C is +/- 0.97 degrees C and for a strain range from 0 to 1100 mu epsilon is +/- 13.04 mu epsilon.