Unbalanced fiber optic Michelson interferometer as an...

Optics: measuring and testing – By light interference

Reexamination Certificate

Rate now

  [ 0.00 ] – not rated yet Voters 0   Comments 0

Details

C356S035500, C356S477000

Reexamination Certificate

active

06317213

ABSTRACT:

BACKGROUND OF THE INVENTION
The present invention relates to optical sensors used to measure changes in environmental parameters such as pressure, displacement, acceleration, and velocity. More specifically, the invention is directed to an optical pick-off as part of an interferometer that can be used in such a sensor.
Michelson or Mach-Zehnder interferometers have been known for use in certain applications, such as acoustic sensors. A description of a Mach-Zehnder interferometer used in an underwater acoustic sensor is contained in, for example, U.S. Pat. No. 5,448,058 to Arab-Sadeghabadi et al.
An optical interferometer of known type includes a pair of optical fibers into which a single source of light directs a light signal. The light signals, guided respectively through the two fibers, follow optical paths of different lengths, producing a phase difference between the two signal beams when the beams are combined. The combined beams may be detected by an optical detector. If the two signal beams have the same polarization state when they are combined, the signals interfere to form a fringe pattern of bright and dark lines that is detected by the optical detector.
Exposing either or both of the fibers to a change in the environmental parameters, such as an acoustic pressure change, changes the fringe pattern that is incident on the optical detector. Such changes in the fringe pattern as detected by the optical detector may be analyzed to measure the changes in the environmental parameters to which the fiber has been exposed. In this manner, the nature of the acoustic waves to which the fiber is exposed may be determined when the interferometer is used in an acoustic sensor.
Mach-Zehnder or Michelson interferometers employed in underwater acoustic sensor (“hydrophone”) systems use tens of meters of optical fiber wrapped on a mandrel. The fiber is stretched and/or contracted to produce a measured phase delay that is proportional to the changes in pressure resulting from acoustic waves. The interferometer has an optical path length mismatch between its two optical legs that is on the order of one meter, to allow the standard functioning and signal processing with a phase-generated carrier. See, for example, Kersey, “Distributed and Multiplexed Fiber Optic Sensors”, in Udd, Ed.,
Fiber Optic Sensors: An Introduction for Engineers and Scientists
, (New York, 1991), pp. 347-363.
Fiber optic interferometric sensor systems, of the types described above, have found favor over piezoelectric hydrophone systems, due to such advantages as immunity to electromagnetic interference (EMI); the ability to locate all electronic and electrical components and systems in the towing vessel, rather than in the underwater environment; and enhanced capabilities for measuring vector quantities. The prior art fiber optic sensor systems, however, are relatively expensive to manufacture. Thus, less expensive alternatives that provide the same advantages over piezoelectric systems have been sought. Batch-processed silicon chip sensors, having a proof mass that is moved in response to changes in environmental parameters, such as pressure and acceleration (which may result from, for example, vehicle or medium motion), have been employed as accelerometers and velocity sensors. Such silicon sensors are very inexpensive and quite rugged. Use of such silicon sensors in a hydrophone system, with the proof mass accessed by a fiber optic delivery system, would lower costs as compared with prior art fiber optic systems. Making such chip sensors compatible with existing fiber optic architectures in Mach-Zehnder and Michelson interferometric sensing systems and the like has, however, proved troublesome in practice.
It would therefore be a significant advancement in the state of the art to provide a fiber optic interferometric sensor system, in a hydrophone or like application, that is capable of employing common, batch-processed silicon sensors.
SUMMARY OF THE INVENTION
The present invention is a measuring system that uses an inexpensive silicon chip sensor in an optical interferometer to measure pressure, velocity, acceleration, or other environmental attributes or parameters. In a preferred embodiment, the sensor includes a movable proof mass that is used as a movable mirror at the end of one leg of an interferometer having two unequal length legs. The proof mass of the silicon chip sensor moves in response to a change in a particular environmental parameter, changing the optical length of the interferometer leg.
The present invention includes an optical signal source for providing a pulsed, coherent light signal, and an interferometer having first and second fiber optic legs of unequal optical path length. The signal is split into first and second beams that are respectively directed into the first and second fiber optic legs. A fixed end mirror is placed on the end of the first of the fiber optic legs for reflecting the first beam received at the end of the first fiber optic leg. An optical pick-off is fixed beyond the end of the second of the fiber optic legs. The optical pick-off comprises a proof mass that is movable relative to the end of the second fiber optic leg. The surface of the proof mass is reflective and positioned to reflect the second beam received from the end of the second fiber leg. An optical coupler combines the first and second beams reflected from the fixed end mirror and the proof mass, producing an interference signal. An optical detector optically coupled to the coupler detects the interference signal of the combined beams and generates an electronic signal having a value indicative of the value of the interference signal. The electronic signal is analyzed to correlate its value to changes in the value of the environmental parameter to be measured.
The measuring system of the present invention provides an accurate, relatively low-cost fiber optic interferometric sensor system, in a hydrophone or like application, that employs common, batch-processed silicon sensors, and that is completely compatible with existing fiber optic architectures of telemetric systems.


REFERENCES:
patent: 4428239 (1984-01-01), Johnston
patent: 4446543 (1984-05-01), McLandrich et al.
patent: 4678909 (1987-07-01), Jackson et al.
patent: 4799797 (1989-01-01), Huggins
patent: 5087124 (1992-02-01), Smith et al.
patent: 5218420 (1993-06-01), Asmar
patent: 5448058 (1995-09-01), Arab-Sadeghabadi et al.
patent: 5505804 (1996-04-01), Furstenau
patent: 5529671 (1996-06-01), Debley et al.
patent: 5675415 (1997-10-01), Akatsu et al.
patent: 5680489 (1997-10-01), Kersey
patent: 5949740 (1999-09-01), Hall
patent: 0196784 (1986-10-01), None
patent: 8-35811 (1996-02-01), None
patent: 09005028 (1997-01-01), None
patent: 2-302632 (1990-12-01), None
patent: 07260617 (1995-10-01), None
patent: 1-237430 (1989-09-01), None
Kersey, “Distributed and Multiplexed Fiber Optic Sensors,” in Udd, Ed.,Fiber OpticSensors: An Introduction for Engineers and Scientists, (New York, 1991), pp. 347-363.

LandOfFree

Say what you really think

Search LandOfFree.com for the USA inventors and patents. Rate them and share your experience with other people.

Rating

Unbalanced fiber optic Michelson interferometer as an... does not yet have a rating. At this time, there are no reviews or comments for this patent.

If you have personal experience with Unbalanced fiber optic Michelson interferometer as an..., we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Unbalanced fiber optic Michelson interferometer as an... will most certainly appreciate the feedback.

Rate now

     

Profile ID: LFUS-PAI-O-2580072

  Search
All data on this website is collected from public sources. Our data reflects the most accurate information available at the time of publication.