Abstract:
An embedded optical sensor has a plurality of layers (10-20) and an optical fiber (21) with a fiber grating (28), disposed between the layers (14, 16). The layers (10-20) comprise filaments (22) and resin (24) which have different thermal expansion coefficients and the filaments (22) are oriented so as to create unequal transverse residual stresses that act through the geometry of a resin-rich region that surrounds on the grating (28) in the fiber (21). The unequal transverse residual stresses cause birefringence in the grating (28), thereby causing the grating (28) to reflect light (32) having two wavelengths with a predetermined separation, each along a different polarization axis. The wavelength separation and average wavelength between such separation have different sensitivities to temperature and strain, thereby allowing independent temperature and strain measurements using only a single grating. The birefringence is maximized when the filaments (22) of the adjacent layers (10, 12) are oriented at 90 degrees with respect to the longitudinal (Z-axis) of the fiber (21).
Abstract:
A sensor employs a laser (12) to obtain a collimated light beam for transmission across the gas effluent of a catalytic cracking process. Particulate matter entrained in the gas flow forward scatters light energy to a collecting aperture (18) which, in turn focuses the scattered light on a first photodetector (22). A second photodetector (30) receives directly transmitted light energy. A ratio (64) between the output signals of the two photodetectors is derived and presented to a threshold level detector (70). If the magnitude of the scatter exceeds a predetermined level it is concluded that a catalyst load dump has occurred. The optical system is carefully selected to ensure that only light energy scattered from a sample volume (16) within the entrained gas flow reaches the first photodetector (22). This is important because it prevents particulate matter on the surfaces of the transparent windows (36 and 50) from affecting the operation of the sensor.
Abstract:
A single polarization fiber and/or amplifier includes a non-polarization preserving fiber (10) having a fiber grating tap (12) which has a predetermined length and strength ( DELTA n/n) and is oriented at a predetermined angle theta and has a grating spacing D so as to couple-out of the fiber (10) a predetermined amount of one polarization (24) over a predetermined wavelength range of an input light (16) and pass the other polarization (28) as output light (26), the grating length being substantially the length of the fiber (10). Alternatively, all or a portion of the fiber (10) may be doped to form a polarization sensitive optical amplifier.
Abstract translation:单个偏振光纤和/或放大器包括具有预定长度和强度(DELTA n / n)并且以预定角度θ定向的光纤光栅抽头(12)的非偏振保留光纤(10) 光栅间隔D,以在输入光(16)的预定波长范围内耦合出光纤(10)预定量的一个偏振(24),并将另一个偏振(28)作为输出光(26)通过, 光栅长度基本上是光纤(10)的长度。 或者,光纤(10)的全部或一部分可以被掺杂以形成偏振敏感的光放大器。
Abstract:
A variable light filtering arrangement (10) includes at least one optical fiber section (11) including a waveguiding core (13), and at least one permanent Bragg grating region (12) in the optical fiber section. The grating region includes a plurality of grating elements constituted by periodic refractive index variations of a predetermined initial periodicity and cumulatively redirecting, of the light launched into the core for guided propagation therein, that having an axial wavelength within a narrow band around a central wavelength that is determined by the periodicity and refractive index variations of the grating elements. At least one of the periodicity and refractive index variations of the grating region is controlledly modified in such a manner as to temporarily change the central wavelength within a predetermined wavelength range.
Abstract:
An optical waveguide mode discrimination light filtering arrangement includes an optical waveguide (10) having an elongated multimode core (11), and a cladding (12) that guides at least two modes of light of a given frequency in an elongated path along a longitudinal axis of said core (11). At least one grating region (13) is embedded in the core (11) at a location remote from the end portions of the core (11) and has a multitude of grating elements (14) extending with a substantially equal longitudinal spacing substantially normal to the longitudinal axis to reflect light propagating in the path and reaching the grating elements (14) back into the path for longitudinal propagation therein opposite to the original propagation direction. The spaceing of the grating elements (14) is so related to the axial wavelength of one of the modes that the reflected light (Rμ) of the one mode interferes constructively while the light (Tμ) of any other of the modes passes through the grating region (13) in the original propagation direction substantially without attenuation.
Abstract:
A polarized fiber laser source includes a fiber laser (10) comprising a pair of Bragg gratings (14, 16) at opposite ends of a fiber laser cavity (18) which is doped with a rare-earth dopant so as to allow lasing to occur at a lasing wavelength lambda L. A grating tap (26) is provided along a portion of the laser cavity (18) to couple-out a predetermined amount of light along one polarization, e.g., the "s" polarization, at the lasing wavelength lambda L. This causes one polarization mode to experience more loss than the other, thereby allowing the fiber laser to lase only on the less lossy polarization mode and causing the laser output light (40) to be polarized only along such polarization.
Abstract:
A remote active multipoint fiber laser sensor includes a plurality of fiber lasers (12, 14, 16), each having a pair of Bragg gratings (18, 20), embedded in a fiber (10) and excited by a common pump light (30). The lasers (12, 14, 16) lase at different longitudinal modes (lasing wavelengths) and emit light (32, 34, 36), at their respective wavelengths ( lambda 1, lambda 2, lambda n). The lasing wavelength of each laser shifts due to perturbations, such as strain or temperature, applied thereto. The output light (32, 34, 36) is fed to a spectrum analyzer (50) where the wavelength shift is analyzed. A signal processor (54) reads the wavelength shift and provides a signal on lines (56) indicative of the perturbation at each of the lasers/sensors (12-16). Alternatively, a single laser may be used as a single sensor. Alternatively, birefringent fiber may be used as the fiber cavities (21) and the two polarizations are beat together to form a lower difference or ''beat'' frequency, thereby allowing lower frequency detection devices to be used.
Abstract:
A method of establishing a dielectric periodic index of refraction phase grating (16) upon the core (19) of an optical waveguide (15) by intense angled application of several tranverse beams (99) of ultraviolet light, enabling the establishment of a distributed, spatially resolving optical fiber strain gauge (13).
Abstract:
A distributed, spatially resolving optical fiber strain gauge (13) in which the core (19) of the optical fiber (15) is written with periodic grating patterns (16) effective for transmitting and reflecting light injected into the core (19). Spectral shifts in the transmitted and reflected light indicate the intensity of strain or temperature variations at positions of the grating (16) corresponding to the associated wavelength of injected light.