EP1896813A2 - Jauge extensometrique optique - Google Patents
Jauge extensometrique optiqueInfo
- Publication number
- EP1896813A2 EP1896813A2 EP06762219A EP06762219A EP1896813A2 EP 1896813 A2 EP1896813 A2 EP 1896813A2 EP 06762219 A EP06762219 A EP 06762219A EP 06762219 A EP06762219 A EP 06762219A EP 1896813 A2 EP1896813 A2 EP 1896813A2
- Authority
- EP
- European Patent Office
- Prior art keywords
- optical
- strain gauge
- bragg grating
- strain
- carrier film
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 103
- 239000013307 optical fiber Substances 0.000 claims abstract description 32
- 239000004033 plastic Substances 0.000 claims abstract description 9
- 229920003023 plastic Polymers 0.000 claims abstract description 9
- 239000000463 material Substances 0.000 claims abstract description 7
- 238000001514 detection method Methods 0.000 claims description 10
- 239000003365 glass fiber Substances 0.000 claims description 10
- 238000000034 method Methods 0.000 claims description 9
- 239000000853 adhesive Substances 0.000 claims description 8
- 230000001070 adhesive effect Effects 0.000 claims description 8
- 238000004519 manufacturing process Methods 0.000 claims description 8
- 239000011521 glass Substances 0.000 claims description 6
- 239000000919 ceramic Substances 0.000 claims description 4
- 238000005530 etching Methods 0.000 claims description 3
- 238000003780 insertion Methods 0.000 claims description 3
- 230000037431 insertion Effects 0.000 claims description 3
- 239000002184 metal Substances 0.000 claims description 2
- 229910052751 metal Inorganic materials 0.000 claims description 2
- 239000010408 film Substances 0.000 description 29
- 239000000835 fiber Substances 0.000 description 21
- 230000001419 dependent effect Effects 0.000 description 10
- 239000010410 layer Substances 0.000 description 9
- 238000005259 measurement Methods 0.000 description 9
- 238000011156 evaluation Methods 0.000 description 7
- 238000005253 cladding Methods 0.000 description 5
- 230000000694 effects Effects 0.000 description 5
- 239000011888 foil Substances 0.000 description 5
- 230000005540 biological transmission Effects 0.000 description 4
- 239000000758 substrate Substances 0.000 description 4
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 3
- 239000002131 composite material Substances 0.000 description 3
- 239000004020 conductor Substances 0.000 description 3
- 239000004038 photonic crystal Substances 0.000 description 3
- 239000004642 Polyimide Substances 0.000 description 2
- 238000004026 adhesive bonding Methods 0.000 description 2
- 238000009529 body temperature measurement Methods 0.000 description 2
- 239000013039 cover film Substances 0.000 description 2
- 238000013461 design Methods 0.000 description 2
- 230000005672 electromagnetic field Effects 0.000 description 2
- 239000003822 epoxy resin Substances 0.000 description 2
- 229910052500 inorganic mineral Inorganic materials 0.000 description 2
- 239000004922 lacquer Substances 0.000 description 2
- 239000011707 mineral Substances 0.000 description 2
- 238000012544 monitoring process Methods 0.000 description 2
- 229920000647 polyepoxide Polymers 0.000 description 2
- 229920001721 polyimide Polymers 0.000 description 2
- 229920000307 polymer substrate Polymers 0.000 description 2
- 239000011241 protective layer Substances 0.000 description 2
- 230000035945 sensitivity Effects 0.000 description 2
- 239000004593 Epoxy Substances 0.000 description 1
- 238000004458 analytical method Methods 0.000 description 1
- 238000005452 bending Methods 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000003486 chemical etching Methods 0.000 description 1
- 229920001940 conductive polymer Polymers 0.000 description 1
- 238000005336 cracking Methods 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 230000018109 developmental process Effects 0.000 description 1
- 239000002360 explosive Substances 0.000 description 1
- 239000013305 flexible fiber Substances 0.000 description 1
- 231100001261 hazardous Toxicity 0.000 description 1
- 238000005342 ion exchange Methods 0.000 description 1
- 230000001678 irradiating effect Effects 0.000 description 1
- 230000000873 masking effect Effects 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 230000000737 periodic effect Effects 0.000 description 1
- 229920002120 photoresistant polymer Polymers 0.000 description 1
- 229920000642 polymer Polymers 0.000 description 1
- 238000003825 pressing Methods 0.000 description 1
- 238000003672 processing method Methods 0.000 description 1
- 230000001681 protective effect Effects 0.000 description 1
- 230000003014 reinforcing effect Effects 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 238000012360 testing method Methods 0.000 description 1
- 238000012546 transfer Methods 0.000 description 1
Classifications
-
- 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 infrared, visible light, ultraviolet
- 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 infrared, visible light, ultraviolet the material being an optical fibre
- G01L1/246—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 infrared, visible light, ultraviolet the material being an optical fibre using integrated gratings, e.g. Bragg gratings
Definitions
- the invention relates to an optical strain gauge according to the preamble of patent claim 1 and its manufacturing method according to the preamble of patent claim 9.
- Such electrical strain gages usually consist of meander-shaped measuring grids produced photolithographically from an electrical resistance material which is applied to a carrier film made of plastic and for mechanical protection, usually with a further one
- These electrical strain gauges are applied to a deformation-dependent strain to detect a load-dependent strain and convert the strain by a change in resistance of the measuring grid in an electrical signal that is proportional to the strain or the force.
- electrical strain gauges are sensitive to electromagnetic fields or high-voltage influence and may not be used in potentially explosive atmospheres.
- a high voltage insensitive optical strain sensor for measuring the contact force of a current collector for rail vehicles is known from DE 102 49 896 Al. This is between the sanding bar and a Holding frame of the current collector attached to an expansion body whose surface deforms according to the contact force.
- a so-called fiber Bragg grating sensor is fixed, which obviously consists of an optical waveguide, in whose application area a so-called Bragg grating is embossed, which changes its reflection wavelength according to the detected strain.
- the waveguide end with the Bragg grating is simply glued to the deformation body and acts as an electrical strain gauge on a load-dependent surface strain.
- An embedded optical sensor is known from EP 753 130 Bl, which consists of a linear waveguide with a Bragg grating embedded within multiple layers of reinforcing filaments to form a laminated structure. This sensor is designed to measure both stresses and temperatures in the structure within the laminated structure with a single Bragg grating fiber.
- a voltage sensor must always be embedded in the measurement object, so that the deformation element must always represent a laminated structure, so that it can not produce thin planar optical strain gauges with comparable dimensions as with electrical strain gauges.
- EP 1 129 327 Bl a sensor for measuring mechanical stresses with fiber-optic Bragg gratings is known, which is designed as a planar flat transducer, which can be applied to a deformation body.
- This voltage sensor is provided as a rosette for measuring a multi-axis voltage, which consists of a waveguide with preferably three successively arranged Bragg gratings, which are aligned at certain angles to each other. To reduce the sensor surface and to avoid larger reflection losses are therefore the curved
- the waveguide with the Bragg gratings and the connecting elements is preferably encapsulated in a rigid epoxy or glued between two parallel rigid plates.
- the plates can be attached to the surface of deformation bodies and thus transfer the strain applied to the plates to the fiber Bragg gratings whose reflected wavelength changes in proportion to the strain and can be detected.
- Optical fiber unrolled over the middle of the row of holes and glued onto the adhesive strip carrier. Thereafter, the adhesive strip with the fixed optical fiber is positioned on the support surface and coated with a lacquer layer that penetrates through the rows of holes and the
- the invention is therefore based on the object to provide prefabricated strain gauges of optical waveguides that can be produced in precise uniform manufacturing quality and can be manufactured inexpensively.
- the invention has the advantage that very compact optical strain gauges can be produced by fixing the waveguide with the Bragg gratings in provided guide channels on a carrier foil.
- the provided guide channels are preferably by a photolithographic etching process or a mechanical processing method made very accurately, so that such optical strain gauges have a high reproducibility and can advantageously be prefabricated as serial parts in large quantities at low cost to be applied in a simple manner on intended deformation bodies or other expansion bodies.
- Such prefabricated flat and small-area optical strain gauges can also be advantageously fixed in or on fiber composites, which affect the fiber structure only slightly and advantageously also withstand strain changes up to 10% undamaged, as are common in deformation bodies made of fiber composites.
- the optical strain gages of the invention have the advantage over electrical strain gauges that they are largely insensitive to electromagnetic fields and high voltage areas. They advantageously have no power supply, so that they are insensitive to power fluctuations on the transmission line and may also be used in hazardous areas. Furthermore, the non-positive connection of the Bragg gratings in the guide channels allows an enclosed connection structure with the flat carrier film, so that a good and defined power transmission is ensured on the Bragg gratings, whereby a high measurement accuracy and in particular a low hysteresis effect can be achieved.
- a particular embodiment of the invention in which the optical waveguides are cast over the entire surface in the guide channels, has the advantage that it can be made very flat easy to manufacture optical strain gauges. Because these optical strain gauges too can be produced from ceramic or glass carrier foils and optical waveguides made of glass materials, these can be advantageously used even at very high temperature loads.
- Strain gauge and the adjacent remaining components can be detected.
- Fig. 1 the top view of an optical
- an optical strain gauge 1 is shown, which is designed for biaxial strain measurement as a rosette and basically consists of three juxtaposed optical waveguides 2, 3, 4 with embossed Bragg gratings 5 in the incorporated guide channels 7, 8, 9 a carrier film 6 are fixed.
- a thin elastic carrier film 6 is provided, which is preferably made of plastic, such as. B. polyimide.
- the carrier film 6 can but also made of other hard elastic plastics, metals, glass or ceramics. In practice, an elastic silica glass film has proven to be very thin and in which the guide channels can be precisely ground.
- the carrier film 6 is used to apply the prefabricated optical strain gauges 1 on provided deformation bodies or to integrate in loaded components in a positionally and non-positively.
- the prefabricated support film 6 is planar, preferably has a rectangular or square base and a thickness of about 0.3 mm. For special designs but also film thicknesses of 0.2 to 0.8 mm are possible.
- the base depends essentially on the length of the Bragg gratings 5 at the ends of the optical waveguides 2, 3, 4 and the formation of the optical strain gauges 1 for one or two-axis strain detections.
- a linearly aligned optical waveguide 3 is provided in a guide channel 2 of the carrier film 6, which has a length of about 8 to 15 mm and a width of about 2 to 5 mm, depending on the required Stör- Nutzsignalabstand.
- an optical strain gauge 1 for biaxial strain detection by means of three angularly offset disposed Bragg gratings 5 a size of the support film 6 of about 26 x 30 mm is provided. The size is determined not only by the 10 mm long Bragg gratings 5, but essentially also by the
- optical waveguide 2, 3, 4 guide channels 7, 8, 9 or recesses incorporated, whose cross section corresponds at least to the cross section of the optical waveguides 2, 3, 4.
- optical waveguides 2, 3, 4 are preferably used made of mineral glass fibers with an outer diameter of 0.25 mm, so that the guide channels 7, 8, 9 or depressions at least in the lead-in area 12 to the cross-sectional edge AA each have a depth and width of 0.25 mm have.
- optical waveguides 2, 3, 4 The arrangement of the optical waveguides 2, 3, 4 is shown in detail in detail in Fig. 2 of the drawing. From the section of the sectional image A-A it can be seen that four optical waveguides 2, 3, 4, 13 are arranged parallel next to one another in the lead-in region 12. There are three
- Optical waveguide 2, 3, 4 provided for strain measurement and an end in the lead-in optical waveguide 13 is used only for temperature compensation.
- This fourth optical waveguide 13 ends about 2 mm behind the introduction edge and has outside the carrier film 6, a Bragg grating 14 for temperature detection.
- the other three optical waveguides 2, 3, 4 are continued after the introduction region 12 only with their fiber cladding region.
- These glass fibers 2, 3, 4 are preferably made of a fiber core 15, a fiber cladding 16 and a fiber protection layer 17, which may also be omitted. Since the optical light-guiding effect occurs exclusively in the core 15 and cladding region 16 of the glass fiber, the fiber protection layer 17 has been removed as a mechanical protection region behind the introduction region 12. This is also necessary in order to impress the Bragg gratings 5 at the end of the glass fibers 2, 3, 4.
- three further guiding channels 7, 8, 9 of only 0.125 mm (or less) depth and width are incorporated into the carrier film 6, which corresponds to the diameter of the fiber jacket 16.
- the middle guide channel 8 for fixing the second optical waveguide 3 extends linearly and simultaneously represents the center line of the symmetrical optical strain gauge 1.
- the second optical waveguide 3 with the two outer optical waveguides 4, 3 in each case an angle of 45 ° and the two outer to each other an angle of 90 °, so that so that all strains in the two surface axes can be detected.
- the optical waveguides 2, 3, 4 are inserted into the three guide channels 7, 8, 9 which are diverging, at the ends of which the three Bragg gratings 5 have already been embossed.
- the three optical fibers 2, 3, 4 are very flexible and with 0.125 mm diameter or less relatively thin, the insertion into the guide channels 7, 8, 9 can be done easily both mechanically and manually, as this by the accurately fitting guide channel dimensions Pressure can be fixed in this. In this case, a firm connection can be achieved both by pressing and by gluing to the carrier film 6, so that not only a form-fitting, but also a firm frictional connection between the optical waveguides 2, 3, 4 and the carrier film 6 takes place.
- a so-called strain gauge rosette is basically formed, with which all horizontally extending force or expansion components can be detected.
- a curable epoxy resin adhesive has been proven in practice, which also has only low hysteresis and excellent transmission of the strain on the optical waveguide 2, 3, 4 guaranteed.
- the optical waveguide 2, 3, 4 is designed as a planar optical waveguide, which is preferably cast in the guide channels 7, 8, 9, 10.
- an optically conductive polymer substrate or another so-called photoresist is introduced into the guide channel 7, 8, 9, 10 of the plastic carrier film 6, which has a higher refractive index than the carrier film 6.
- the polymer substrate is basically the core and the carrier film 6 the sheath with the lower refractive index.
- the light line of certain wavelengths as glass fibers is suitable.
- strip-shaped irregularities are imprinted at a distance ⁇ before introducing the photoconductive layer into the guide channels 7, 8, 9, which then act as Bragg gratings 5.
- These can represent comb-like elevations or depressions which form a Bragg grating over a length L of 3 to 10 mm, which reflects the light waves fed in at a predetermined wavelength ⁇ B. Because the
- Optical waveguides 2, 3, 4 firmly embedded in the guide channels 7, 8, 9 of the support layer 6 and are firmly connected to these, so that all strains acting on the support layer 6 can be accurately detected.
- these polymeric optical waveguides 2, 3, 4 as optical strip conductors, very flat designs of optical strain gauges 1 which are thinner than 0.5 mm can be realized.
- Such embodiments of optically conductive media embedded in the guide channels 7, 8, 9 as optical waveguides 2, 3, 4 can also be carried out with heat-resistant glass or ceramic films as carrier layer 6, in whose guide channels 7, 8, 9 photonic crystals are cast with quartz glass substrates.
- the Bragg gratings are formed with the help of photonic crystals, with which the strain is detected.
- the channels can preferably also be realized by a field-assisted ion exchange.
- the Bragg gratings are then introduced into these channels from outside through a chemical etching process.
- Such embodiments of optical strain gauges 1 can be used at temperatures up to 900 0 C. .._
- the guide channels 7, 8, 9, 10 are additionally coated with the inserted waveguides 2, 3, 4 with a thin cover film 19.
- the cover 19 is preferably also made of the material of the carrier film 6 such. As polyimide and preferably has a thickness of 0.05 mm and is welded or glued to the support sheet 6, so that the optical strain gauge 1 is hermetically sealed.
- Such an optical strain gauge 1 can be applied both to metallic deformation bodies as conventional electrical strain gauges or inserted or glued in fiber composites. With such optical strain gauges 1 are not only strain measurements, but also
- optical strain gauge 1 If such an optical strain gauge 1 is applied to a force-loaded deformation body, it can thus be described as follows, the applied force or strain can be detected. Because of the force acting on the expansion body force takes place on the surface of an expansion effect, which is transmitted via the applied thereto carrier sheet 6 on the non-positively fixed therein optical waveguides 2, 3, 4. This also creates a change in length within the Bragg grating region L, since this is formed from a piece of the core 15 of the optical fiber 2, 3, 4, which is surrounded by the shell 16, which has a lower refractive index than the core 15.
- the optical fiber 2, 3, 4 is formed above as a single-mode fiber in which the diameter of the 9 ⁇ m fiber core 15 is sufficiently small so that the light from a preferably infrared light source can propagate along the core 15 in only a single mode. This single mode is essentially guided by the refractive index jump at the core-cladding boundary.
- the lines 20 of the Bragg grating 5 are a series of preferably regularly spaced perturbations of the effective refractive index n of the core 15.
- the Bragg grating 5 extends along a length L of the optical fiber 2, 3, 4, where L is normally in the range of 3 up to 20 mm.
- the refractive indices n in the core 15 are generated by masking the optical fibers 2, 3, 4 with a phase mask and irradiating them with strong ultraviolet light.
- the index perturbations n are formed by exposing the optical fibers 2, 3, 4 to an interference pattern generated from two intersecting halves of a UV laser beam. The distance ⁇ between the index perturbations n is determined by the angle at which the two halves of the beam intersect.
- the Bragg gratings 5 are formed by disturbances in the carrier film 6.
- a comb-like line pattern is mechanically impressed into the carrier film 6 with the distance ⁇ , through which the light waves are reflected.
- the Bragg grating 5 is preferably formed by irradiation with UV light and a phase mask. The disturbances caused by these methods Nuclear refractive index n is usually on the order of one-thousandth or less.
- the optical fibers 2, 3, 4 used for the production of Bragg gratings 5 generally have a protective layer 17 outside of the jacket 16, which preferably consists of a polymer and has no significance for the actual light-guiding function. This protective layer 17 is removed before the optical fiber 2, 3, 4 is exposed to the UV light to form the Bragg grating 5. After irradiation, the stripped portion of the optical fiber 2, 3, 4 may also be recoated to restore its durability. However, since the optical fibers 2, 3, 4 in the present exemplary embodiment run in the guide channels 7, 8, 9 and are protected by both the carrier film 6 and the cover film 19, sufficient mechanical protection of the optical fibers 2, 3 is provided in the optical strain gauge 1 according to the invention , 4 guaranteed.
- the Bragg grating 5 When the Bragg grating 5 is supplied with a broad spectrum of light as an input signal, most wavelengths penetrate the grating area and form a transmitted output signal. The periodic disturbances of the refractive index n, however, produce a strong Bragg reflection with components of the input signal
- the lightwave signals reflected by the Bragg grating 5 can be detected.
- the determined wavelength ⁇ at which a peak occurs in reflection, a value which is dependent on the grating period ⁇ .
- a longitudinal strain acts on the Bragg grating 5 changes the distance ⁇ , so that the Bragg wavelength ⁇ B shifts.
- the Bragg wavelength ⁇ B behaves approximately proportionally to the strain along the longitudinal axis of the optical waveguides 2, 3, 4.
- the wavelength change ⁇ B is thus a measure of the introduced into the deformation body
- optical strain gauges 1 can be used similarly to electrical strain gauges on provided deformation body preferably in load cells, torque shafts or other force transducers.
- optical strain gauges 1 can be used similarly to electrical strain gauges on provided deformation body preferably in load cells, torque shafts or other force transducers.
- Strain gauges 1 also used in load tests, for example in aerospace, where the optical strain gauges 1 are then applied directly to the loaded components, in particular the rosettes according to the invention for measuring the unknown force introduction directions are useful. But also for monitoring the operating state of loaded components such optical strain gauges 1 can be used, which can detect a fatigue damage or cracking when exceeding a predetermined limit strain.
- this evaluation unit 21 contains a transmitting and receiving unit 23 for optical waveguides 2, 3, 4, in which the evaluation unit 21 detects the wavelength ⁇ B reflected by the Bragg gratings 5, 14. It is first in the unloaded state by means of a preferably infrared light source as
- K E the sensitivity factor of the elongation
- ⁇ the strain
- K ⁇ the sensitivity factor of the temperature
- ⁇ T the temperature change.
- a fourth optical waveguide 13 with Bragg grating 14 located outside the optical strain gauge 1 additionally becomes provided for temperature compensation.
- the fourth optical waveguide 13 could also be integrated into the carrier foil 6 in the case of a modified optical strain gauge 1. Then, however, the associated guide channel 10 would have to be dimensioned such that the Bragg grating 14 rests loosely to exclude the effects of stretching.
- Such an additional optical fiber with a Bragg grating 14 for temperature compensation is also provided for linear optical strain gauges 1 with only a straight optical fiber 3. It can be the additional Optical fiber are also used simultaneously to a pure temperature measurement.
- optical strain gauges 1 can be formed, in which a plurality of rosettes or a plurality of linear optical fibers are arranged on a larger support film surface, which allow a flat strain detection, to determine an analysis of the voltage curve, for example, on complicated components.
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Length Measuring Devices By Optical Means (AREA)
- Optical Transform (AREA)
- Light Guides In General And Applications Therefor (AREA)
Abstract
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE200510030751 DE102005030751A1 (de) | 2005-06-29 | 2005-06-29 | Optischer Dehnungsmessstreifen |
PCT/EP2006/006214 WO2007000324A2 (fr) | 2005-06-29 | 2006-06-27 | Jauge extensometrique optique |
Publications (1)
Publication Number | Publication Date |
---|---|
EP1896813A2 true EP1896813A2 (fr) | 2008-03-12 |
Family
ID=37440640
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP06762219A Withdrawn EP1896813A2 (fr) | 2005-06-29 | 2006-06-27 | Jauge extensometrique optique |
Country Status (3)
Country | Link |
---|---|
EP (1) | EP1896813A2 (fr) |
DE (1) | DE102005030751A1 (fr) |
WO (1) | WO2007000324A2 (fr) |
Families Citing this family (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE102006002500B4 (de) * | 2006-01-13 | 2008-02-28 | Hottinger Baldwin Messtechnik Gmbh | Optisches Spektrometer |
DE102007007047A1 (de) | 2007-02-08 | 2008-08-14 | Hottinger Baldwin Messtechnik Gmbh | Vorrichtung zur Erfassung von Schwingungen oder Durchbiegungen von Rotorblättern einer Windkraftanlage |
DE102008027931A1 (de) * | 2008-06-12 | 2010-01-07 | Hottinger Baldwin Messtechnik Gmbh | Optischer Dehnungssensor |
DE102009018927A1 (de) | 2009-04-28 | 2010-11-04 | Deutsche Bahn Ag | Vorrichtung zur Messung der zwischen Rad und Schiene auftretenden Kräfte, insbesondere Messradsatz für Schienenfahrzeuge |
DE102011084579B4 (de) | 2011-10-14 | 2013-11-07 | Bauhaus Universität Weimar | Vorrichtung und Verfahren zur Überwachung des Zustands einer Klebverbindung |
DE102013219149A1 (de) | 2013-09-24 | 2015-04-09 | Schaeffler Technologies AG & Co. KG | Messsystem und Messverfahren zur Messung einer Oberflächendehnung mittels eines plasmonischen Reflektors |
CN104613890B (zh) * | 2015-02-09 | 2017-04-19 | 清华大学 | 光栅应变测量装置 |
DE102018108399B4 (de) * | 2018-04-10 | 2024-02-29 | Dr. Ing. H.C. F. Porsche Aktiengesellschaft | Kraftfahrzeugkarosserieelement mit einem Formüberwachungssystem für eine Kraftfahrzeugkarosserie |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4750796A (en) * | 1985-05-31 | 1988-06-14 | Sumitomo Electric Industries, Ltd. | Optical sensor |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2727203B1 (fr) * | 1994-11-18 | 1996-12-13 | Commissariat Energie Atomique | Micro-systeme optique de type rosette de jauges de contraintes a guides dielectriques pour la mesure d'une contrainte longitudinale en structure plane |
US6778735B2 (en) * | 2001-03-19 | 2004-08-17 | Micron Optics, Inc. | Tunable fiber Bragg gratings |
-
2005
- 2005-06-29 DE DE200510030751 patent/DE102005030751A1/de not_active Withdrawn
-
2006
- 2006-06-27 EP EP06762219A patent/EP1896813A2/fr not_active Withdrawn
- 2006-06-27 WO PCT/EP2006/006214 patent/WO2007000324A2/fr not_active Application Discontinuation
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4750796A (en) * | 1985-05-31 | 1988-06-14 | Sumitomo Electric Industries, Ltd. | Optical sensor |
Also Published As
Publication number | Publication date |
---|---|
WO2007000324A2 (fr) | 2007-01-04 |
DE102005030751A1 (de) | 2007-01-11 |
WO2007000324A3 (fr) | 2007-03-22 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
EP1899700B1 (fr) | Jauge extensometrique optique | |
EP1122528B1 (fr) | Arrangement et méthode pour déterminer dilatations et températures et ses variations d'une couche de couverture appliquée sur un support | |
DE69912301T2 (de) | Sensor zur messung mechanischer spannungen mit fiber-optischen bragg gittern | |
WO2007000324A2 (fr) | Jauge extensometrique optique | |
DE102016100432B4 (de) | Automatisch vorgespannte und vollständig von einer Feder ummantelte Lichtleiter-Sensorstruktur | |
DE69636019T2 (de) | Integriert-optischer interferometrischer Sensor | |
EP2126511B1 (fr) | Jauge optique d'allongement | |
DE2819590A1 (de) | Vorrichtung zur messung der in einem festen koerper vorliegenden spannung | |
EP1134566A1 (fr) | Procédé pour mesurer la température à l'aide d'un fibre optique et capteur de température à fibre optique | |
EP0342192B1 (fr) | Capteur optique de mesure de force | |
DE102011050717B4 (de) | Messsystem und Verfahren zum Validieren eines faseroptischen Sensor | |
DE3418247A1 (de) | Durchbiegungsmesser | |
DE102011084579B4 (de) | Vorrichtung und Verfahren zur Überwachung des Zustands einer Klebverbindung | |
DE3608599C2 (fr) | ||
EP2812667B1 (fr) | Dispositif de mesure et procédé pour détecter la sollicitation de force d'un objet souple en flexion | |
DE102012221067A1 (de) | Dehnungsmessstreifen und mechanische Komponente | |
EP2294374B1 (fr) | Capteur optique d allongement | |
EP2926104A2 (fr) | Procédé de mesure de pression à résolution spatiale | |
DE102017201523A1 (de) | Faseroptische Erfassungseinrichtung sowie Verfahren zum Betreiben einer solchen faseroptischen Erfassungseinrichtung | |
WO2019180161A1 (fr) | Capteur de température | |
WO2015024915A1 (fr) | Module de détection | |
DE3701548A1 (de) | Optischer kraftmessensor | |
DE19755739A1 (de) | Lichtwellenleiter-Dehnungsmeßstreifen (LWL-DMS) |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
17P | Request for examination filed |
Effective date: 20071220 |
|
AK | Designated contracting states |
Kind code of ref document: A2 Designated state(s): AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HU IE IS IT LI LT LU LV MC NL PL PT RO SE SI SK TR |
|
DAX | Request for extension of the european patent (deleted) | ||
RIN1 | Information on inventor provided before grant (corrected) |
Inventor name: HAASE, KARL-HEINZ Inventor name: SCHMIDT, MICHAEL Inventor name: BLIN, REGIS |
|
DAX | Request for extension of the european patent (deleted) | ||
17Q | First examination report despatched |
Effective date: 20090420 |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE APPLICATION IS DEEMED TO BE WITHDRAWN |
|
18D | Application deemed to be withdrawn |
Effective date: 20160823 |