Jia et al., 2019 - Google Patents
Fiber optic dual-ring michelson interferometer-based detection scheme for the measurement of dynamic signalsJia et al., 2019
- Document ID
- 7155069866970370916
- Author
- Jia J
- Jiang Y
- Zhang L
- Gao H
- Jiang L
- Publication year
- Publication venue
- Journal of Lightwave Technology
External Links
Snippet
A fiber optic dual-ring Michelson interferometer (DRMI) based detection scheme for the measurement of dynamic signals is proposed and experimentally demonstrated. The fiber optic sensor is a single mode fiber between two broadband fiber Bragg gratings (FBGs) with …
- 239000000835 fiber 0 title abstract description 39
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
- G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infra-red, visible, or ultra-violet light
- G01D5/32—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infra-red, visible, or ultra-violet light with attenuation or whole or partial obturation of beams of light
- G01D5/34—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infra-red, visible, or ultra-violet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
- G01D5/353—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infra-red, visible, or ultra-violet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B9/00—Instruments as specified in the subgroups and characterised by the use of optical measuring means
- G01B9/02—Interferometers for determining dimensional properties of, or relations between, measurement objects
- G01B9/02055—Interferometers for determining dimensional properties of, or relations between, measurement objects characterised by error reduction techniques
- G01B9/02075—Interferometers for determining dimensional properties of, or relations between, measurement objects characterised by error reduction techniques of particular errors
- G01B9/02078—Caused by ambiguity
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B9/00—Instruments as specified in the subgroups and characterised by the use of optical measuring means
- G01B9/02—Interferometers for determining dimensional properties of, or relations between, measurement objects
- G01B9/02001—Interferometers for determining dimensional properties of, or relations between, measurement objects characterised by manipulating or generating specific radiation properties
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
- G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infra-red, visible, or ultra-violet light
- G01D5/266—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infra-red, visible, or ultra-violet light by interferometric means
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01H—MEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
- G01H9/00—Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means
- G01H9/004—Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means using fibre optic sensors
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B9/00—Instruments as specified in the subgroups and characterised by the use of optical measuring means
- G01B9/02—Interferometers for determining dimensional properties of, or relations between, measurement objects
- G01B9/02049—Interferometers for determining dimensional properties of, or relations between, measurement objects characterised by particular mechanical design details
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L1/00—Measuring force or stress in general
- G01L1/24—Measuring force or stress in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infra-red, visible light, ultra-violet
- G01L1/242—Measuring force or stress in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infra-red, visible light, ultra-violet the material being an optical fibre
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L11/00—Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00
- G01L11/02—Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00 by optical means
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L9/00—Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by electric or magnetic pressure-sensitive elements; Transmitting or indicating the displacement of mechanical pressure-sensitive elements, used to measure the steady or quasi-steady pressure of a fluid or fluent solid material by electric or magnetic means
- G01L9/0001—Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means
- G01L9/0008—Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means using vibrations
- G01L9/0019—Transmitting or indicating the displacement of elastically deformable gauges by electric, electro-mechanical, magnetic or electro-magnetic means using vibrations of a semiconductive element
- G01L9/002—Optical excitation or measuring
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01P—MEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
- G01P15/00—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration
- G01P15/02—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses
- G01P15/08—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values
- G01P15/097—Measuring acceleration; Measuring deceleration; Measuring shock, i.e. sudden change of acceleration by making use of inertia forces using solid seismic masses with conversion into electric or magnetic values by vibratory elements
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B2290/00—Aspects of interferometers not specifically covered by any group under G01B9/02
Similar Documents
Publication | Publication Date | Title |
---|---|---|
Li et al. | Ultra-high sensitive quasi-distributed acoustic sensor based on coherent OTDR and cylindrical transducer | |
Jia et al. | Fiber optic dual-ring michelson interferometer-based detection scheme for the measurement of dynamic signals | |
Liu et al. | Diaphragm based long cavity Fabry–Perot fiber acoustic sensor using phase generated carrier | |
Lin et al. | A high-resolution fiber optic accelerometer based on intracavity phase-generated carrier (PGC) modulation | |
Murray et al. | Fiber-wrapped mandrel microphone for low-noise acoustic measurements | |
Guo et al. | Ultrahigh sensitivity fiber-optic Fabry–Perot interferometric acoustic sensor based on silicon cantilever | |
Zhang et al. | Fiber-optic micro vibration sensors fabricated by a femtosecond laser | |
Yang et al. | Wideband fiber-optic Fabry-Perot acoustic sensing scheme using high-speed absolute cavity length demodulation | |
Wang et al. | Optical fiber acoustic sensor based on nonstandard fused coupler and aluminum foil | |
Jiang et al. | Noncontact ultrasonic detection in low-pressure carbon dioxide medium using high sensitivity fiber-optic Fabry–Perot sensor system | |
Jia et al. | Dual-wavelength DC compensation technique for the demodulation of EFPI fiber sensors | |
Jia et al. | Phase demodulator for the measurement of extrinsic Fabry-Perot interferometric sensors with arbitrary initial cavity length | |
Liu et al. | A compact fiber optic Fabry–Perot sensor for simultaneous measurement of acoustic and temperature | |
Shi et al. | Single-wavelength passive phase-shifted demodulation technique with the dual-cavity and EFA for the interrogation of EFPI diaphragm-based fiber sensor | |
Guo et al. | High-sensitivity fiber-optic low-frequency acoustic detector based on cross-correlation demodulation | |
Fu et al. | Fiber-based large dynamic range vibration sensing with dual-wavelength phase unwrapping | |
WO2014096784A1 (en) | Mechanical resonator sensor | |
US11796383B2 (en) | Ultrasound detection based on phase shift | |
Huang et al. | Ultra-high-resolution phase demodulation based miniature fiber-optic accelerometer at low and medium frequencies | |
Jia et al. | Symbiosis-Michelson interferometer-based detection scheme for the measurement of dynamic signals | |
Niu et al. | Fiber Fabry–Pérot hydrophone based on push–pull structure and differential detection | |
Sathitanon et al. | A fiber optic interferometric sensor for dynamic measurement | |
Guo et al. | Non-contact fiber vibration sensor based on intracavity modulation of an extrinsic Fabry–Perot interferometer | |
Wu et al. | A novel optical accelerometer based on slant-ended fiber | |
Pullteap | Development of an optical fiber based interferometer for small vibration measurements |