SE413344B - OPTICAL METDON - Google Patents
OPTICAL METDONInfo
- 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
Links
- 230000003287 optical effect Effects 0.000 title claims 2
- 239000000835 fiber Substances 0.000 claims description 35
- 230000004907 flux Effects 0.000 claims description 7
- 230000007423 decrease Effects 0.000 claims description 2
- 230000001133 acceleration Effects 0.000 claims 1
- 230000005855 radiation Effects 0.000 claims 1
- 241000489861 Maximus Species 0.000 description 1
- 210000000481 breast Anatomy 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 239000000523 sample Substances 0.000 description 1
- 239000004065 semiconductor Substances 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
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)
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)
Country | Link |
---|---|
SE (1) | SE413344B (en) |
Cited By (1)
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 |
-
1978
- 1978-03-17 SE SE7803086A patent/SE413344B/en not_active IP Right Cessation
Cited By (1)
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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