Abstract:Kvantovaya Elektron. (Moscow) 12, 901-944 (May 1985)Optical, fiber-optic, and integrated optical sensors of physical effects are reviewed. The sensors are classified in accordance with their operating principle: amplitude, interference, and polarization sensors are considered. Descriptions are given of the construction of the sensors (or of their sensitive elements) which can react to mechanical quantities (displacement, force, acceleration), acoustic vibrations and pressure, electric and magnetic fields, elec… Show more
“…Density (g/cm³) 1.1 (1) 3.19 (1) Total Transmission (%) 91.28 (2) internal transmittance at 546 nm (10 mm): 99.8 (1) Coefficient of thermal expansion [m/(mK)]…”
Section: Materials Propertymentioning
confidence: 99%
“…Fiber optic temperature sensing enables monitoring in particular surroundings such as microwaves or explosion sensitivity [1][2][3][4]. Commercially, available fiber optic temperature sensors often use a semiconductor-chip, which has an absorption edge that moves with the temperature [5,6].…”
This paper describes the development and function of an optical fiber temperature sensor made out of a compound of epoxy and optical glass particles. Because of the different thermo-optic coefficients of these materials, this compound exhibits a strong wavelength and temperature dependent optical transmission, and it therefore can be employed for fiber optic temperature measurements. The temperature at the sensor, which is integrated into a polymer optical fiber (POF), is evaluated by the ratio of the transmitted intensity of two different light-emitting diodes (LED) with a wavelength of 460 nm and 650 nm. The material characterization and influences of different sensor lengths and two particle sizes on the measurement result are discussed. The temperature dependency of the transmission increases with smaller particles and with increasing sensor length. With glass particles with a diameter of 43 µm and a sensor length of 9.8 mm, the intensity ratio of the two LEDs decreases by 60% within a temperature change from 10℃ to 40℃.
“…Density (g/cm³) 1.1 (1) 3.19 (1) Total Transmission (%) 91.28 (2) internal transmittance at 546 nm (10 mm): 99.8 (1) Coefficient of thermal expansion [m/(mK)]…”
Section: Materials Propertymentioning
confidence: 99%
“…Fiber optic temperature sensing enables monitoring in particular surroundings such as microwaves or explosion sensitivity [1][2][3][4]. Commercially, available fiber optic temperature sensors often use a semiconductor-chip, which has an absorption edge that moves with the temperature [5,6].…”
This paper describes the development and function of an optical fiber temperature sensor made out of a compound of epoxy and optical glass particles. Because of the different thermo-optic coefficients of these materials, this compound exhibits a strong wavelength and temperature dependent optical transmission, and it therefore can be employed for fiber optic temperature measurements. The temperature at the sensor, which is integrated into a polymer optical fiber (POF), is evaluated by the ratio of the transmitted intensity of two different light-emitting diodes (LED) with a wavelength of 460 nm and 650 nm. The material characterization and influences of different sensor lengths and two particle sizes on the measurement result are discussed. The temperature dependency of the transmission increases with smaller particles and with increasing sensor length. With glass particles with a diameter of 43 µm and a sensor length of 9.8 mm, the intensity ratio of the two LEDs decreases by 60% within a temperature change from 10℃ to 40℃.
“…That is, first.the mechanical deformation of the fiber is converted into an optical phase shift (e.g., radians per gram or radians per micrometer), then the optical phase shift is converted into an analogous electrical signal by an interferometric demodulator, which consists of photodiodes, amplifiers, signal processing electronics, etc., to produce a given voltage per radian of optical phase shift. Although both of these processes introduce noise into the measurement, only the electrooptic demodulation noise has been treated in the literature [ 11 , [2], [5] , [9]-[ 1 11. This deficiency has not caused any difficulty to date because the optical sensitivity of the sensors has not been large and most sensor systems have been plagued by other noise problems and measurements in low noise environments have not been attempted.…”
Section: Intrinsic (Thermal) Noise and Minimum Detectable Signalmentioning
confidence: 99%
“…The promise of high sensitivity was not based on the intrinsic sensitivity of optical fibers to physical stimuli but on the fact that optical phase shifts on the order of microradians could be resolved and optical path lengths of tens or hundreds of meters could be incorporated in sensors of modest physical dimensions. That combination of high interferometric demodulator resolution and long optical path length led to the possibility of measurements with resolutions on the order of a part in 10" to In addition to measurement of conventional physical parameters [l], [2] such as temperature, pressure, etc. , fiber-optic sensors were suggested for such unusual measurements as the detection of cosmologically generated gravitational waves [3].…”
Abstract-A fiber-optic interferometric sensor has been developed which consists of a seismic mass of 520 gm supported by two rubber mandrels, each wound with a single layer of single-mode optical fiber 6.5 m long. One end of each fiber is cleaved to enhance reflection. The other ends are interconnected via a fiber-to-fiber 3-dB coupler, forming a Michelson interferometer. When the case of the sensor is displaced, the fiber around one mandrel extends in length while the other contracts. The resulting "push-pull" mechanical operation of the sensor allows both legs of the interferometer to be active, providing good common mode rejection of spurious effects, as a reference leg is not required. This, together with the fact that the light traverses each leg of a Michelson interferometer twice due to reflection, provides the sensor with four times the sensitivity of a conventionally constructed interferometric sensor. sensitivities of 8500 rad of optical phase shift per micrometer of case displacement have been measured above the massspring resonance, where the sensor operates as a seismometer. Below resonance the sensor operates as an accelerometer with a measured sensitivity of 10 500 rad/g, the highest reported to date. Including both thermodynamic and demodulator noise sources ( = 10 p r a d / J H z ) , below resonance the sensor has a detection threshold of l ng/JHz, a 20-dB improvement over the best existing conventional low noise vibration sensors.M
“…Many optical fiber sensors have been developed based on amplitude or phase techniques [1]. Different interferometric configurations have been proposed as temperature sensors such as Mach-Zehnder [2] and Fabry-Perot [3].…”
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