SE413344B - OPTICAL METDON - Google Patents

OPTICAL METDON

Info

Publication number
SE413344B
SE413344B SE7803086A SE7803086A SE413344B SE 413344 B SE413344 B SE 413344B SE 7803086 A SE7803086 A SE 7803086A SE 7803086 A SE7803086 A SE 7803086A SE 413344 B SE413344 B SE 413344B
Authority
SE
Sweden
Prior art keywords
light
fiber
measuring device
fibers
initiating
Prior art date
Application number
SE7803086A
Other languages
Swedish (sv)
Other versions
SE7803086L (en
Inventor
T Brogardh
Original Assignee
Asea Ab
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Asea Ab filed Critical Asea Ab
Priority to SE7803086A priority Critical patent/SE413344B/en
Publication of SE7803086L publication Critical patent/SE7803086L/en
Publication of SE413344B publication Critical patent/SE413344B/en

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING 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
    • G01D5/00Mechanical 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
    • G01D5/26Mechanical 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
    • G01D5/268Mechanical 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

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Light Guides In General And Applications Therefor (AREA)

Description

10 15 -20 25 30 das 1803086-5 utledande fibrerna.. Summan användes för stabiliserixzg av det från lysdioden utsända ljuset medan skillnaden utgör mätdonets mätsignal. 10 15 -20 25 30 das 1803086-5 the sum was used to stabilize it from the LED emit the light while the difference is the measuring signal of the measuring device.

Föremšlet för föreliggande tilläggspetent utgöres av en modifikation sv det ovan' beskrivna mätdonet." Liksom .vid det kända mätdonet omfattar uppfinningsföre-f man: :vs anar, sem s: mömngs 1 förhållande :in maximus. m Iam-mama fibern är anordnad i den ena delen och de ljuutledßnde fibrerna i den andra. ïad som i öfvrigt kännetecknar uppfinningen framgår avpatentkraven.The subject matter of the present additional patent consists of a modification sv it As described in the known measuring device, the present invention comprises man:: vs anar, sem s: mömngs 1 relationship: in maximus. m Iam-mama the fiber is arranged in one part and the light-emitting fibers in the other. ïad which otherwise characterizes the invention appear from the patent claims.

I På. bifogad ritning visar fig den till mätdond: hörande elektriska. utrustningen samt (le-optiska. fibremn. Fig 2 v-isar en skäm anordnad på. en genomskinlig skiva mellan sändande och mottagen-ide fibrer. Fig 5 visar en skärm anordnad på den ljusinledsnde fibern då. denna har större area. än de ljusutledande eller mottagande fibrerna. ' I fig 1 är den ljusinledande eller sändande fibernbeteoknad 1 och de ljusut- ledande eller mottagande fibrerna betecknade 2 och 3. Em lysdiod 4, alternativt ' halvledarlaeer, är anordnad ett sända in ljus i fibern 1 och intensiteten av det utsända' ljuset styres av ett styrdon 7. Det genom de mottagande fibrema. 2 resp Ékommande ljusflödet faller på fotodiodernay 5 resp 6, vara fotoströmmar förstärks :L elektronikenheterna 8 resp 9. De från dessa. enheter erhållna sigm- lerna. påföras två. suzmneringsdon 10 resp 11, vilka bildar sunmnn resp skillnaden av de båda. signalerna., Smnmssignslen från donet 10 påföres styrdonet 7, som styr lysdioden 4, så. datt ettpkonstant szmmaljusflöde erhålles till fotodioderns 5 an. 6. skmmaassigmsism :man smemimgmaemet 11 maxar» m instrument 12, som kan vara :mammas eller seglen-emma snar ma. utför: pa met lämpligt sätt. i ' såalvm mamaemsm Omfattar tva delar, som 1 rig 1 är betecknade med zo gon 25.In On. the attached drawing shows the figure belonging to the measuring probe: electrical. the equipment and (le-optical. fiber belt. Fig. 2 shows a core arranged on. a transparent disc between transmitting and received fibers. Fig. 5 shows a screen arranged on the light-initiating fiber then. this has a larger area. than the light emitting or receiving the fibers. ' In Fig. 1, the light-initiating or transmitting fiber bait 1 and the light-emitting conductive or receiving fibers designated 2 and 3. Em LED 4, alternatively ' semiconductor layers, a transmitting light is arranged in the fiber 1 and the intensity of the emitted light is controlled by a control device 7. It through the receiving fibers. 2 resp The incoming light flux falls on photodiode nays 5 and 6, respectively, be photocurrents reinforced: L electronics units 8 and 9 respectively. Those from these. units received sig- lerna. applied two. summing means 10 and 11, respectively, which form the sun and the difference, respectively of the two. the signals., The signal from the device 10 is applied to the control device 7, which control LED 4, then. that a constant beam light flux is obtained to the photodiodes 5 an. 6. skmmaassigmsism: man smemimgmaemet 11 maxar »m instrument 12, which can be: mammas or seglen-emma snar ma. perform: pa met appropriate way. i ' såalvm mamaemsm Comprises two parts, which 1 rig 1 are denoted by zo gon 25.

Den sändande fibern 1 är infäst i delen 20 och de "båda mottagande fibrernß _ 2 och ä är ínfästa. :L delen 25. Hur infästningen är utförd i detalj är 'beski- vet i hnvudpatentet och förbigâs därför här. Vidare antagee här, ett delen 20 är rörlig relativt delen 25. _ Fig 2 visa: fibrernss ändgtor. Em genomskinlig skiva 17 är anordnad så. att lju- set frân fibern 1 komer ut genom ett horisontellt fält 19. 'De streokede ytorna 18 är skärmande partier hos den genomskinlig. skivan. Fibern är rörlig i hori- sonten lea, se sem ambbupiiem 16 utvisar. om dem samasmeefium 1 rör sig dt vinster i figuren, kommer ljusflödet in i. den mottagande fiborn 2 ett minska. samtidigt som ljusflödot in i fibern 5 ökar. Summan av de blåa. mottagna ljus- flödena. förblir konstant, medan 'skillnaden mellan dem ökar. Resultatet blir en minskning av utsignalen från summeringsdonet 11. uThe transmitting fiber 1 is attached to the part 20 and the "two receiving fibers" 2 and ä are attached. : L part 25. How the attachment is made in detail is' described know in the main patent and are therefore overlooked here. Further assume here, a part 20 is movable relative to the part 25. _ Fig. 2 shows: end ends of the fibers. A transparent disc 17 is arranged so. to sound set from the fiber 1 emerges through a horizontal field 19. 'The stroked surfaces 18 are shielding portions of the transparent. the disc. The fiber is mobile in horizontal sonten lea, se sem ambbupiiem 16 utvisar. if them samasmee fi um 1 moves dt gains in the figure, the luminous flux enters the receiving fiber 2 a decrease. at the same time as the light flux into the fiber 5 increases. The sum of the blues. received light the flows. remains constant, while the 'difference between them increases. The result is one reduction of the output signal from the summing device 11. u

Claims (5)

10 7803086-3 Fig 3 visar ett mätdon, i vilket den sändande fibern 1 har en diameter, som är i huvudsak dubbelt så. stor som de. mottagande fibrernas 2 och 5 diameter. Den sändande fiberns ändyta är skärmad till en stor del, vilket är markerat strecket. Endast två vertikala fält 13 är ljusgenomsläppande, så att ljus kan falla in i de båda mottagande fibrerna.. Vid denna utföringsform av mätdonet är fibern 1 rör- lig i vertikal led, vilket markeras med dubbelpilen 20. När den eändande fibern bringas att röra sig uppåt av en yttre kraft, minskar det ljusflöde, som går in i den mottagande 'fibern 2, medan ljusflödet in i den vänstra fibern 3 ökar i motsvarande grad. ' K De visade sk dels på. fiberänden, dels på. en separat skiva är att anse endast som exempel på hur en yttre kraft eller rörelse kan styra ljusflö- det från den sändande fibern in i de mottagande fibrerna.. Ytterligare utförings- former är tänkbara. _ PATENTKIAVFig. 3 shows a measuring device in which the transmitting fiber 1 has a diameter which is substantially twice as large. big as they are. the diameter of the receiving fibers 2 and 5. The end surface of the transmitting fiber is largely shielded, which is marked by the line. Only two vertical fields 13 are light transmissive, so that light can fall into the two receiving fibers. In this embodiment of the measuring device, the fiber 1 is movable in vertical direction, which is marked with the double arrow 20. When the end fiber is caused to move upward by an external force, the luminous flux entering the receiving fiber 2 decreases, while the luminous flux entering the left fiber 3 increases correspondingly. 'K They showed so-called partly on. fiber end, partly on. a separate disc is to be considered only as an example of how an external force or movement can control the luminous flux from the transmitting fiber into the receiving fibers. Further embodiments are conceivable. _ PATENTKIAV 1. Optiskt mätdon enligt patentkravat 1 i patentet 7713207-4 för användning vid mätning av fysikaliska storheter som läge, acceleration, kraft, tryck, flödes- haetighet, temperatur etc, och omfattande en företa del (20) och en andra del (25) samt ljusinledande och ljusutledande fibrer (1, 2, 5), Åk å. n n e t e o k -y n a d därav, att"-'de ljusinledande fibrerna (1) är anordnade i mäfdonetg första del och de ljusutledande fibrerna (2, S) är anordnade i mätdonets andra del. 2". nataon enlig: patenzmm, 1, k e n n e t a c k n aa sei-av, at: inataonefs båda delar med ljusledande fibrer är så, anordnade, att åtminstone en del ev lju- set från aan ljuasnleaanaa fiber-n (1) kan men; direkt 1 ae 'ljusuflaamae rib-An optical measuring device according to claim 1 of patent 7713207-4 for use in measuring physical quantities such as position, acceleration, force, pressure, flow rate, temperature, etc., and comprising an integral part (20) and a second part (25) and light-initiating and light-emitting fibers (1, 2, 5), in addition to the fact that the light-initiating fibers (1) are arranged in the first part and the light-conducting fibers (2, S) are arranged in the measuring device. second part. 2 ". nataon according to: patenzmm, 1, k e n n e t a c k n aa sei-av, that: inataonefs both parts with light-conducting fibers are so arranged that at least some of the light from aan ljuasnleaanaa fiber-n (1) can men; directly 1 ae 'light fl aamae rib- 1381738.1381738. 5. Mätdon enligt patentlmavet 1, k ä n n e t e c k n ad därav, att en skärm (15, 17) är anordnad i strdlgåxxgen mellan de ljusinledande och de ljusutledande fibrerna: ändytor.5. Measuring device according to claim 1, characterized in that a screen (15, 17) is arranged in the radiation path between the light-initiating and the light-emitting fibers: end surfaces. 4. Mätdon enligt patentkraven 1 och 5, k ä. n n e t e c k n a d därav, att skärmen (15) är fäst vid den del av mätdonet, som innehåller den ljusinledande fibßrnoMeasuring device according to Claims 1 and 5, characterized in that the screen (15) is attached to the part of the measuring device which contains the light-initiating fiber. 5. Mätdon enligt patentkravet 5, k ä n n e t e c k n a. d därav, att skärmen är utformad genom slipning och stening av den ljusinledande fiberns ändyta. - ANFÖRDA PUBLIKATIONER: Sverige 355 080 (G01R 21/06) TySkLand 2 345 498 (G01D 5/58), 2 509 112 (6028, 5/16), 2 733 281 (G02B 5/14) ' -Measuring device according to Claim 5, characterized in that the screen is formed by grinding and stoning the end surface of the light-initiating fiber. PUBLICATIONS REFERRED TO: Sweden 355 080 (G01R 21/06) GERMANY 2 345 498 (G01D 5/58), 2 509 112 (6028, 5/16), 2 733 281 (G02B 5/14) '-
SE7803086A 1978-03-17 1978-03-17 OPTICAL METDON SE413344B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
SE7803086A SE413344B (en) 1978-03-17 1978-03-17 OPTICAL METDON

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
SE7803086A SE413344B (en) 1978-03-17 1978-03-17 OPTICAL METDON

Publications (2)

Publication Number Publication Date
SE7803086L SE7803086L (en) 1979-09-18
SE413344B true SE413344B (en) 1980-05-19

Family

ID=20334349

Family Applications (1)

Application Number Title Priority Date Filing Date
SE7803086A SE413344B (en) 1978-03-17 1978-03-17 OPTICAL METDON

Country Status (1)

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Cited By (1)

* Cited by examiner, † Cited by third party
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

Cited By (1)

* Cited by examiner, † Cited by third party
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

Also Published As

Publication number Publication date
SE7803086L (en) 1979-09-18

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