Method of making a distributed optical fiber sensor having enhanced Rayleigh scattering and enhanced temperature stability, and monitoring systems employing same
11467338 · 2022-10-11
Assignee
Inventors
- Peng Kevin Chen (Pittsburgh, PA, US)
- Aidong Yan (Pittsburgh, PA, US)
- Michael P. Buric (Pittsburgh, PA, US)
- Paul R. Ohodnicki (Allison Park, PA)
- Sheng Huang (Pittsburgh, PA, US)
Cpc classification
G02B6/0229
PHYSICS
G02B6/02204
PHYSICS
G01M11/37
PHYSICS
Y02P70/50
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
G02B6/02147
PHYSICS
Y02E60/50
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
H01M8/04067
ELECTRICITY
G02B6/29319
PHYSICS
G01M11/3172
PHYSICS
International classification
H01M8/12
ELECTRICITY
G01M11/00
PHYSICS
Abstract
A method of making an optical fiber sensor device for distributed sensing includes generating a laser beam comprising a plurality of ultrafast pulses, and focusing the laser beam into a core of an optical fiber to form a nanograting structure within the core, wherein the nanograting structure includes a plurality of spaced nanograting elements each extending substantially parallel to a longitudinal axis of optical fiber. Also, an optical fiber sensor device for distributed sensing includes an optical fiber having a longitudinal axis, a core, and a nanograting structure within the core, wherein the nanograting structure includes a plurality of spaced nanograting elements each extending substantially parallel to the longitudinal axis of the optical fiber. Also, a distributed sensing method and system and an energy production system that employs such an optical fiber sensor device.
Claims
1. A method of making an optical fiber sensor device structured for distributed sensing, comprising: generating a laser beam comprising a plurality of ultrafast pulses; and focusing the laser beam into a core of an optical fiber to form a nanograting structure within the core, wherein the nanograting structure includes a plurality of spaced nanograting elements each extending substantially parallel to a longitudinal axis of optical fiber, wherein the nanograting elements each extend in a first direction that is substantially parallel to the longitudinal axis of the optical fiber, wherein the nanograting elements are spaced in a periodic manner from one another and aligned and positioned immediately adjacent one another in a second direction that is substantially perpendicular to the first direction, and wherein there is no spacing between or within any of the nanograting elements in the first direction such that the core does not include any grating elements therein spaced from one another in the first direction.
2. The method according to claim 1, wherein the plurality of ultrafast pulses comprises a plurality of femtosecond ultrafast pulses.
3. The method according to claim 2, wherein each of the femtosecond ultrafast pulses is a sub-μJ laser pulse.
4. The method according to claim 1, further comprising causing the laser beam and the optical fiber to be moved relative to one another during focusing such that the nanograting structure is formed within a longitudinally extending portion of the core.
5. The method according to claim 4, wherein a position of the laser beam in a longitudinal direction is stationary and wherein the optical fiber is caused to move relative to the laser beam.
6. The method according to claim 4, wherein the optical fiber is stationary and wherein the laser beam is caused to move relative to the optical fiber.
7. The method according to claim 1, wherein a portion of the core surrounding the nanograting structure has a first refractive index and wherein each nanograting element has a second refractive index that is lower than the first refractive index.
8. The method according to claim 7, wherein the second refractive index is 99% to 90% of the first refractive index.
9. The method according to claim 1, wherein each nanograting element is generally planar and has a length that extends in the first direction, a width that extends in the second direction, and a height that extends in a third direction that is substantially perpendicular to the longitudinal axis of the optical fiber.
10. The method according to claim 9, wherein the optical fiber sensor device is designed for use with an interrogating light having a wavelength, and wherein a spacing between each pair of immediately adjacent nanograting elements is less than or equal to one-fifth of the wavelength of the interrogating light.
11. The method according to claim 9, wherein the optical fiber sensor device is designed for use with an interrogating light having a wavelength, and wherein a spacing between each pair of immediately adjacent nanograting elements is less than or equal to one-tenth of the wavelength of the interrogating light.
12. The method according to claim 9, wherein a spacing between each immediately adjacent pair of nanograting elements is 750 nm or less.
13. The method according to claim 1, wherein the optical fiber is a single-crystal optical fiber.
14. The method according to claim 13, wherein the optical fiber is a sapphire: optical fiber.
15. The method according to claim 1, further comprising annealing the optical fiber sensor device after the formation of the nanograting structure in the presence of a reactive gas.
16. The method according to claim 15, wherein the reactive gas is hydrogen.
17. The method according to claim 15, wherein the annealing is performed at a temperature that is greater than or equal to 700° C.
18. The method according to claim 17, wherein the annealing is performed at a temperature that is greater than or equal to 800° C.
19. The method according to claim 15, wherein the annealing causes a plurality of voids to be formed within the core.
20. The method according to claim 15, wherein the annealing causes a plurality of voids to be formed at least partially within each of the nanograting elements.
21. The method according to claim 20, wherein each of the voids is spherical.
Description
BRIEF F DESCRIPTION OF THE DRAWINGS
(1)
(2)
(3)
(4)
(5)
DETAILED DESCRIPTION OF EXEMPLARY EMBODIMENTS
(6) As used herein, the singular form of “a” “an”, and “the” include plural references unless the context clearly dictates otherwise.
(7) As used herein, the statement that two or more parts or components are “coupled” shall mean that the parts are joined or operate together either directly or indirectly, i.e., through one or more intermediate parts or components, so long as a link occurs.
(8) As used herein, “directly coupled” means that two elements are directly in contact with each other.
(9) As used herein, the term “number” shall mean one or an integer greater than one (i.e., a plurality).
(10) As used herein, the term “ultrafast pulse” shall mean an electromagnetic pulse whose time duration is on the order of one nanosecond or less.
(11) As used herein, the term “ultrafast laser system” shall mean a laser system that generates and emits laser pulses that are ultrafast pulses.
(12) As used herein, the term “femtosecond ultrafast pulse” shall mean an ultrafast pulse whose time duration is on the order of 500 femtoseconds or less.
(13) As used herein, the term “femtosecond ultrafast laser system” shall mean an ultrafast laser system that generates and emits laser pulses that are femtosecond ultrafast pulses.
(14) As used herein, the term “substantially parallel” shall mean exactly parallel or within ±10° of exactly parallel.
(15) As used herein, the term “substantially perpendicular” shall mean exactly perpendicular or within ±10° of exactly perpendicular.
(16) Directional phrases used herein, such as, for example and without limitation, top, bottom, left, right, upper, lower, front, back, and derivatives thereof, relate to the orientation of the elements shown in the drawings and are not limiting upon the claims unless expressly recited therein.
(17) The disclosed concept will now be described, for purposes of explanation, in connection with numerous specific details in order to provide a thorough understanding of the disclosed concept. It will be evident, however, that the disclosed concept can be practiced without these specific details without departing from the spirit and scope of this innovation.
(18) As described in greater detail herein, the disclosed concept uses ultrafast (e.g., femtosecond) laser irradiation with sub-μJ laser pulses (e.g., 300-nJ laser pulses) to produce optical fiber sensor devices that have enhanced Rayleigh scattering profiles and that are stable at high (e.g., 400° C. and higher) temperatures.
(19) The resultant enhanced optical fiber sensor devices can, in the exemplary embodiment, perform distributed temperature sensing with very small (e.g., 1 mm) spatial resolution at very high temperatures (e.g. 800° C.) in highly reactive fuel gas (e.g., hydrogen) streams. Using this powerful sensing tool, distributed temperature measurements may be performed in harsh environments such as, without limitation, an operating SOFC system. In particular, in certain exemplary embodiments, infoiniation gathered by the optical fiber sensor devices of the disclosed concept can be compared with simulation results to aid in SOFC system design, or used to perform in-vivo monitoring of an active cell, and ultimately improve the operational efficiency and longevity of SOFC systems (or other energy production systems).
(20)
(21) Nanograting structure 6 is the mechanism that enables optical fiber sensor device 4 of the disclosed concept to provide enhanced Rayleigh scattering profiles and to be stable at high temperatures. As seen in
(22) In one particular, non-limiting exemplary embodiment, the spacing between each pair of immediately adjacent nanograting elements 12 is significantly smaller than (in one particular embodiment less than or equal to one-fifth of) the wavelength of the interrogating light that is to be used to interrogate optical fiber sensor device 4 when in use. In another particular, non-limiting exemplary embodiment, the spacing between each pair of immediately adjacent nanograting elements 12 is less than or equal to one-tenth of the wavelength of the interrogating light that is to be used to interrogate optical fiber sensor device 4 when in use. These embodiments are produced via alteration of the ultrafast laser wavelength. These embodiments will reduce the likelihood that interrogation wavelength dependent loss features will be present during use.
(23) Furthermore, in another particular, non-limiting exemplary embodiment, the spacing between each immediately adjacent pair of nanograting elements 12 is 750 nm or less, or, alternatively, 500 nm or less or 250 nm or less. In any case, the height and width of nanograting elements 12 depends on the laser energy deposited into the focal volume, which is also determined by the laser scanning speed.
(24) Referring again to
(25) While in the embodiment just described optical fiber 10 is moved relative to a stationary laser beam 16, it will be appreciated that instead the laser beam may be moved relative to a stationary optical fiber 10 without departing from the scoped the disclosed concept.
(26) In addition, in the embodiment just described, optical fiber 10 is a cylindrical fiber having a cylindrical core 8 and cylindrical cladding surrounding core 8. Alternatively, optical fiber 10 may be a so called D-shaped fiber or a so-called solid-core photonic bandgap fiber.
(27) Moreover, in one non-limiting exemplary embodiment, ultrafast laser system 14 is a Coherent ferntosecond ultrafast laser system that consists of a Coherent MIRA-D Ti:sapphire seed oscillator and a RegA 9000 regenerative amplifier operated at 800 nm with a repetition rate of 250 kHz. In this exemplary implementation, the pulse width of laser beam 16 is 300-fs. Also in this exemplary embodiment, the output of cylindrical lenses 18 is focused using an 80× microscope objective.
(28) In addition, the exemplary system 2 as just described was used by the present inventors to create a number of exemplary optical fiber sensor devices 4 in 20 cm long sections of a silica based optical fiber 10 that was translated over 20 cm by motion stage 20 by varying the translation speed of motion stage 20 from 0.1 mm/s to 1 minis Specifically, scanning speeds of 0.1 mm/s, 0.5 mm/s, and 1 mm/s were used to create three exemplary optical fiber sensor devices 4.
(29) According to a further aspect of the disclosed concept, optical fiber sensor device 4 as described herein may be subjected to an annealing process in order to further increase the stability thereof. In particular, in the exemplary embodiment, optical fiber sensor device or is annealed in a tube furnace during a process wherein the temperature of the furnace is ramped up from room temperature to a very high temperature, such as 800° C., in air and held at that temperature for a predetermined period of time, such as 4 hours. Thereafter, the optical fiber sensor device 4 is subjected to a reactive gas mixture, such as a gas mixture including hydrogen (e.g. 10% hydrogen), at the high temperature. In this embodiment, the high temperature annealing in the presence of a reactive gas causes a plurality of voids or nanopores 52 (e.g., spherical voids) to be formed in the core 8 of optical fiber 10 as shown in
(30) Another feature of optical fiber sensor device 4 is the fact that the backscattered amplitude will be different for the s and p polarizations of the backscattered signal. In other words, the backscattered amplitude of optical fiber sensor device 4 is polarization dependent. Such polarization dependence is caused by the anisotropy of nanograting elements 12. This feature can potentially be used for extracting additional value from nanograting elements 12, such as multi-parameter analysis due to the birefringence of the structures.
(31) As noted elsewhere herein, optical fiber sensor device 4 of the disclosed concept may be used to perform distributed sensing (e.g., distributed temperature sensing) in harsh, high temperature environments such as those employed in various energy production processes from biomass reactors, to SOFC systems to nuclear reactors, among others.
(32) Referring to
(33) As seen in
(34) Accordingly, by employing ultrafast (e.g., femtosecond) laser irradiation with sub-μJ pulses, the Rayleigh scattering profile from commercially available silica fibers can be enhanced by more than 50-dB through nanograting formations in the fiber core. This increases the available measurable intensity at the optical detectors of an OFDR system, leading to significant improvements in both the
(35) Signal to noise ratio (SNR) and spectral shift quality of an OFDR-based measurement. The new Rayleigh backscatter features induced by the laser irradiation technique of the disclosed concept are stable at high temperatures, which enables
(36) reliable temperature measurements in extreme environments. This technique therefore represents a powerful new tool to potentially study a wide range of energy production processes from biomass reactors, to solid oxide fuel cells, to monitoring in nuclear reactors. Using the distributed sensing tool of the disclosed concept, reliable temperature measurements can be achieved from room temperature to 800° C. or higher. The disclosed concept may thus be used to probe an operating SOFC's temperature dependence on fuel stream inlet chemistry and fuel utilization that was previously inaccessible using known techniques. The capability for in-situ temperature monitoring with high spatial resolution within operational energy conversion devices such as solid oxide fuel cells represents a significant opportunity for process efficiency and long-term stability, which are two key metrics required for enabling widespread deployment of SOFCs in the power generation sector. The system described herein may also be useful for measurements in existing harsh-environment energy systems including combustion systems, boilers, and gas turbines. Other spatially resolved measurements, such as, without limitation, spatially resolved strain measurements or spatially resolved chemical composition measurements, are also possible within the scope of the disclosed concept.
(37) In the claims, any reference signs placed between parentheses shall not be construed as limiting the claim. The word “comprising” or “including” does not exclude the presence of elements or steps other than those listed in a claim. In a device claim enumerating several means, several of these means may be embodied by one and the same item of hardware. The word “a” or “an” preceding an element does not exclude the presence of a plurality of such elements. In any device claim enumerating several means, several of these means may be embodied by one and the same item of hardware. The mere fact that certain elements are recited in mutually different dependent claims does not indicate that these elements cannot be used in combination.
(38) Although the invention has been described in detail for the purpose of illustration based on what is currently considered to be the most practical and preferred embodiments, it is to be understood that such detail is solely for that purpose and that the invention is not limited to the disclosed embodiments, but, on the contrary, is intended to cover modifications and equivalent arrangements that are within the spirit and scope of the appended claims. For example, it is to be understood that the present invention contemplates that, to the extent possible, one or more features of any embodiment can be combined with one or more features of any other embodiment.