SE410521B - METGIVARE WITH OPTICAL FIBER - Google Patents
METGIVARE WITH OPTICAL FIBERInfo
- Publication number
- SE410521B SE410521B SE7801965A SE7801965A SE410521B SE 410521 B SE410521 B SE 410521B SE 7801965 A SE7801965 A SE 7801965A SE 7801965 A SE7801965 A SE 7801965A SE 410521 B SE410521 B SE 410521B
- Authority
- SE
- Sweden
- Prior art keywords
- fiber
- detector
- transmitter
- parts
- point
- Prior art date
Links
- 239000013307 optical fiber Substances 0.000 title claims description 4
- 239000000835 fiber Substances 0.000 claims description 34
- 230000005855 radiation Effects 0.000 claims description 7
- 239000000463 material Substances 0.000 claims description 2
- NOQGZXFMHARMLW-UHFFFAOYSA-N Daminozide Chemical compound CN(C)NC(=O)CCC(O)=O NOQGZXFMHARMLW-UHFFFAOYSA-N 0.000 claims 1
- 239000004020 conductor Substances 0.000 claims 1
- 230000003287 optical effect Effects 0.000 claims 1
- 230000000630 rising effect Effects 0.000 claims 1
- 238000005259 measurement Methods 0.000 description 2
- 239000000356 contaminant Substances 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 239000002360 explosive Substances 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
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 infrared, visible, or ultraviolet light
- G01D5/268—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 infrared, visible, or ultraviolet light using optical fibres
-
- 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
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Radiation Pyrometers (AREA)
Description
15 20 25 30 35 7801965 -0 kan givarens mätområde och noggrannhet anpassas för olika tillämpningsområden. 15 20 25 30 35 7801965 -0 the sensor's measuring range and accuracy can be adapted for different application areas.
Användningen av optiska fibrer medfiör även andra fördelar. Givaren blir okäns- ng för erekfineka oçh Navman fan. man får galvanisk ieoiation manen givare och mätenhet. Givaren kan användas i explosiv miljö utan några speciella säkerhetsarrangemang. Inga möjliçxeter för gnistbildning eller kortslutning fin- fnes. Mätgivarens fiber utgör ett slutet system. Smuts och andra föroreningar kan ej inverka på. mätresultatet.The use of optical fibers also has other advantages. The sensor becomes insensitive to erek fi neka oçh Navman fan. one gets galvanic ieoiation manen sensor and unit of measurement. The sensor can be used in an explosive environment without any special safety arrangements. There are no possibilities for sparking or short-circuiting. The fiber of the measuring sensor constitutes a closed system. Dirt and other contaminants can not affect. the measurement result.
Vad som i övrigt- kännetecknar uppfinningen framgår av patentkraven.What otherwise characterizes the invention is stated in the claims.
Uppfinningen kommer att förklaras med hjälp av bifogade ritningsfigxlrer.The invention will be explained with the aid of the accompanying drawing figures.
Fig 1 visar uppfinningens princip.Fig. 1 shows the principle of the invention.
Fig 2 visar krökningens amplitud och våglängd. i Fig' 3 visar sambandet mellan dämpning och amplitud för en viss fiber vid olika mekaniska våglängden' i *i -m- * I Fig 4; visar ett enkelt utförande av en deformationszon. K I Fig 5, 6 och 7 visar en givare med ett utökat antal deformationszoner.Fig. 2 shows the amplitude and wavelength of the curvature. in Fig. 3 shows the relationship between attenuation and amplitude for a certain fiber at different mechanical wavelengths' in * i -m- * In Fig. 4; shows a simple design of a deformation zone. K Figs. 5, 6 and 7 show a sensor with an increased number of deformation zones.
Fig 8' visar en riktningsoberoende deformaticnsgivare.Fig. 8 'shows a direction-independent deformation sensor.
Fig 9. visar. en givare med ett svängbart ok.Fig. 9. shows. a sensor with a swivel yoke.
Fig 10 visarenJ givare med temperaturkompensering.Fig. 10 shows the sensor with temperature compensation.
Fig 11 och 12 visar temperaturgivare.Figures 11 and 12 show temperature sensors.
Fig 13 visar ett alternativt arrangemang av sändare och mottagare.Fig. 13 shows an alternative arrangement of transmitter and receiver.
Fig 1» visar principen för en kraftgivare enligt uppfinningen. Em strålninge- källa 1, exempelvis en lasersändare utsänder ljus genomen optisk fiber 2 av multimodetyp eller singlemodetyp och företrädesvis bestående av en kärna omgiven av' en mantel. En detektor 5 är anordnad att mottaga och detektera den ljusstrål- ning, som passerat genom fiberns kärna. En anordning för att deformera fibern består generellt av två. delar 4 och 5 mellan vilka fibern passerar. De båda delarna är utformade med var sin vågformad yta 6, 7, som är vända mot varandra och företrädesvis så, att den ena delens våg-toppar ligger mitt för den andra delens vågdelar. När de båda delarna 4 och 5 tryckas mot varandra med en kraft F kommer fibern att krökas. Krökningen har en våglängd/L, som är lika med av- ståndet mellan två våg-toppar och lcrölmingens amplitud x beror på. de båda de- larnas inbördes läge. våglängd och amplitud visas i fig 2. Fig 5 visar det i en viss fiber rådande sambandet mellan dämpningen eC och amplituden x vid olika mekaniska. våglängder. Kurvonza för våglängd anger från vänster till höger ökande våglängder . __r?- 10 15 20 25 50 35 7801965-0 Fig 4 visar en deformationsanordning, i vilken fibern 2 passerar endast en gång genom anordningen. Fig 5 visar att fibern passerar deformationsanordningen ett flertal gånger. Den kan därvid grara lindad nmt den ena. delen ett antal varv. Fig 6 visar att fibem är lindad fram och tillbaka i slingor. Vid ut- föringsformen enligt fig 7 är delen 4 utförd som en ram, som omsluter den andra delen 5. Fibern 2 kan här med fördel lindas omkring delen 5 ett antal varv.Fig. 1 »shows the principle of a power sensor according to the invention. If a radiation source 1, for example a laser transmitter, emits light through optical fiber 2 of multimode type or single mode type and preferably consisting of a core surrounded by a sheath. A detector 5 is arranged to receive and detect the light radiation which has passed through the core of the fiber. A device for deforming the fiber generally consists of two. parts 4 and 5 between which the fiber passes. The two parts are formed with their respective corrugated surface 6, 7, which face each other and preferably so that the wave peaks of one part lie opposite the wave parts of the other part. When the two parts 4 and 5 are pressed against each other with a force F, the fiber will bend. The curvature has a wavelength / L, which is equal to the distance between two wave peaks and the amplitude x of the curvature depends on. the mutual position of the two parts. wavelength and amplitude are shown in Fig. 2. Fig. 5 shows the relationship prevailing in a certain fiber between the attenuation eC and the amplitude x at different mechanical ones. wavelengths. Curvonza for wavelength indicates from left to right increasing wavelengths. Fig. 4 shows a deformation device, in which the fiber 2 passes only once through the device. Fig. 5 shows that the fiber passes the deformation device several times. It can then be wound wound around one of them. part a number of turns. Fig. 6 shows that the fiber is wound back and forth in loops. In the embodiment according to Fig. 7, the part 4 is designed as a frame, which encloses the second part 5. The fiber 2 can here advantageously be wound around the part 5 a number of turns.
Därigenom erhålles en längre deformerad zon av fiber-n, vilket ger givaren större känslighet. Fig 8 visar utförandet av en givare, som är oberoende av den på.- verkande kraftens riktning. Den yttre delen 4 är utformad som en cylindrisk ring med våg-formad inneryta, medan delen 5 är utformad som en cylinder med våg- formad ytteryta. och placerad inuti delen 4. Fibern 2 är lindad ett antal varv runt innerdelen S. Om ytterdelen göres elastisk kan givaren användas för mät- ning av allsidigt tryck.Thereby a longer deformed zone of the fiber is obtained, which gives the sensor greater sensitivity. Fig. 8 shows the design of a sensor which is independent of the direction of the actuating force. The outer part 4 is designed as a cylindrical ring with a wavy inner surface, while the part 5 is designed as a cylinder with a wavy outer surface. and placed inside the part 4. The fiber 2 is wound a number of turns around the inner part S. If the outer part is made elastic, the sensor can be used for measuring versatile pressure.
Fig' 9 visar en givare med två. av varandra oberoende anordningar för deformering av fibrer. Sändaren 1 utsänder strålning genom två olika fibrer 2a och 2b och vardera fibern passerar sin egen deformationsanordning med delarna 49., Sa resp 4b, 5b. vardera fibern har sin egen detektor ša resp šb. Utsigzalerna från de- tektorerna går till ett summeringsdon 6, som bestämmer skfillnadert mellan sigxa- lerna. Ett U-format ok 7 har livet 8 lagrat i en axel 9 vid livets mitt och flänsanza 10a resp 10b anliggande mot var sin deformationsgivare. Om kraften F verkar nedåt på. flänsen 10a kommer en lika stor lcraft att verka uppåt på. flän- sen 10b. Den vänstra fibern 2a kommer således att bli utsatt .för en avsevärt större deformation än den högra fibern 2b, vilket medför att signalen från de- tektom ja. blir mindre signalen från šb.Fig. 9 shows a sensor with two. independent devices for deforming fibers. The transmitter 1 emits radiation through two different fibers 2a and 2b and each fiber passes its own deformation device with the parts 49., Sa respectively 4b, 5b. each fiber has its own detector ša resp šb. The output cells from the detectors go to a summing device 6, which determines the difference between the signals. A U-shaped yoke 7 has the web 8 mounted in a shaft 9 at the center of the web and flange edges 10a and 10b, respectively, abutting each of the deformation sensors. If the force F acts downwards on. the flange 10a will have an equal force acting upwards on. flange 10b. The left fiber 2a will thus be subjected to a considerably larger deformation than the right fiber 2b, which means that the signal from the detector yes. becomes smaller the signal from šb.
Fig 10 visar en givare med temperaturkompensering. Ett block 11, som är utsatt för den kraft, som skall mätas, innehåller en deformationsanordning 12a för fibern 2a och en andra deformationsanordning 12b för fibern 2b. Anordningen 12a är så orienterad, att den kan påverkas av kraften F, medan den andra deforma- tionsanordnmgen 12b är vriden 90° och är därmed i huvudsak opåverkad av kraf- ten F. När kraften F = 0 skall utsigzalerna från de båda detektoreama Ba och Bb vara lika. I suxmneringsdonet 6 bestämmes skillnaden mellan de båda signalerna..Fig. 10 shows a sensor with temperature compensation. A block 11, which is subjected to the force to be measured, contains a deformation device 12a for the fiber 2a and a second deformation device 12b for the fiber 2b. The device 12a is oriented so that it can be actuated by the force F, while the second deformation device 12b is rotated 90 ° and is thus substantially unaffected by the force F. When the force F = 0, the output cells from the two detector arms Ba and Bb be equal. In the transmitter 6, the difference between the two signals is determined.
Summeringsdonets utsigrzal blir därmed temperaturoberoende.The output of the summing device thus becomes temperature-independent.
I Fig 11 visar en temperaturkännande givare. De båda delarna 4 och 5 är vid sina ändar förbundna med varandra medelst förbindningselement 15 av ett material med hög temperaturutvidguaingskoefficient. Om elementen 13 har positiv temperatur- koefficient ges fibern en viss förspäzming, som minskar vid stigande temperatur när elementen 15 ökar i längd. Fig 12 visar en annan temperaturgivare, i vilkenFig. 11 shows a temperature sensing sensor. The two parts 4 and 5 are connected to each other at their ends by means of connecting elements 15 of a material with a high coefficient of temperature expansion. If the elements 13 have a positive temperature coefficient, the fiber is given a certain bias, which decreases with increasing temperature as the elements 15 increase in length. Fig. 12 shows another temperature sensor, in which
Claims (3)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
SE7801965A SE410521B (en) | 1978-02-21 | 1978-02-21 | METGIVARE WITH OPTICAL FIBER |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
SE7801965A SE410521B (en) | 1978-02-21 | 1978-02-21 | METGIVARE WITH OPTICAL FIBER |
Publications (2)
Publication Number | Publication Date |
---|---|
SE7801965L SE7801965L (en) | 1979-08-22 |
SE410521B true SE410521B (en) | 1979-10-15 |
Family
ID=20334053
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
SE7801965A SE410521B (en) | 1978-02-21 | 1978-02-21 | METGIVARE WITH OPTICAL FIBER |
Country Status (1)
Country | Link |
---|---|
SE (1) | SE410521B (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0096262A1 (en) * | 1982-05-27 | 1983-12-21 | Takaoka Electric Co., Ltd. | Fibre-optic sensor for measuring dynamic quantities |
DE3628715A1 (en) * | 1985-11-14 | 1987-05-21 | Battelle Development Corp | FIBER OPTICAL PRESSURE DETECTOR |
WO1990012283A1 (en) * | 1989-04-10 | 1990-10-18 | Quality Measurement Device Ab | A device for measuring the length of a contact surface |
-
1978
- 1978-02-21 SE SE7801965A patent/SE410521B/en unknown
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0096262A1 (en) * | 1982-05-27 | 1983-12-21 | Takaoka Electric Co., Ltd. | Fibre-optic sensor for measuring dynamic quantities |
DE3628715A1 (en) * | 1985-11-14 | 1987-05-21 | Battelle Development Corp | FIBER OPTICAL PRESSURE DETECTOR |
WO1990012283A1 (en) * | 1989-04-10 | 1990-10-18 | Quality Measurement Device Ab | A device for measuring the length of a contact surface |
Also Published As
Publication number | Publication date |
---|---|
SE7801965L (en) | 1979-08-22 |
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