[go: up one dir, main page]

GB2223841A - Parameter measurement using refractive index change - Google Patents

Parameter measurement using refractive index change Download PDF

Info

Publication number
GB2223841A
GB2223841A GB8820537A GB8820537A GB2223841A GB 2223841 A GB2223841 A GB 2223841A GB 8820537 A GB8820537 A GB 8820537A GB 8820537 A GB8820537 A GB 8820537A GB 2223841 A GB2223841 A GB 2223841A
Authority
GB
United Kingdom
Prior art keywords
parameter
refractive index
temperature
transducer
changes
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Withdrawn
Application number
GB8820537A
Other versions
GB8820537D0 (en
Inventor
Christopher Davies
Robert Marc Clement
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Red Kite Technology Ltd
Original Assignee
Red Kite Technology Ltd
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 Red Kite Technology Ltd filed Critical Red Kite Technology Ltd
Priority to GB8820537A priority Critical patent/GB2223841A/en
Publication of GB8820537D0 publication Critical patent/GB8820537D0/en
Priority to PCT/GB1989/001012 priority patent/WO1990002322A1/en
Priority to AU41914/89A priority patent/AU4191489A/en
Publication of GB2223841A publication Critical patent/GB2223841A/en
Withdrawn legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L11/00Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00
    • G01L11/02Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00 by optical means
    • 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
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01KMEASURING TEMPERATURE; MEASURING QUANTITY OF HEAT; THERMALLY-SENSITIVE ELEMENTS NOT OTHERWISE PROVIDED FOR
    • G01K11/00Measuring temperature based upon physical or chemical changes not covered by groups G01K3/00, G01K5/00, G01K7/00 or G01K9/00
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/41Refractivity; Phase-affecting properties, e.g. optical path length
    • G01N21/43Refractivity; Phase-affecting properties, e.g. optical path length by measuring critical angle
    • G01N21/431Dip refractometers, e.g. using optical fibres

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Measuring Temperature Or Quantity Of Heat (AREA)

Abstract

The apparatus comprises a receptacle for holding a quantity of reference material having known variation of refractive index with changes in the test parameter (which may be temperature, pressure or the like); an elongate optical waveguide in contact with the reference material which is itself in thermal contact (in the case of temperature measurement) or under the same pressure (in the case of pressure measurement); and means for measuring the transmission of light passed along the optical waveguide, so as to provide a measurement depending on the value of the parameter of the reference material and thus of the test material.

Description

Parameter Measurement using Refractive Index Change Ihe present invention relates to the measurement of a parameter of a material using refractive index changes induced by changes in the aforementioned parameter.
It is known to measure and indicate or record the refractive index of various liquids by detecting the attenuation of internally reflected light passing through a transparent optical waveguide, such as a glass rod, an optical fibre or the like.
Optical fibres generally have a central core, entirely surrounded by a plastics or glass sheath (the cladding). In order for optical transmission along such a fibre to take place, the refractive index of the core must be greater than that of the cladding. It is well known that the relative refractive index of the core and cladding will determine the transmission characteristics of light along the optical fibre.
According to one aspect of the present invention, there is provided apparatus for measuring a parameter of a test material through changes in the refractive index thereof produced by or related to changes in said parameter, including an elongate optical waveguide along which light is passed by internal reflection, the waveguide having at least one portion in optical contact with said material and in which the transverse cross section of the said portion has a straight side.
Preferably the cross section of the said portion is polygonal and conveniently rectangular or square.
lhe straight sided or polygonal cross section may extend for substantially the whole length of the waveguide.
According to another aspect of the invention, there is provided apparatus for measuring a parameter of material, including a container holding a quantity of selected material having known variation of refractive index thereof with changes in said parameter, means for subjecting the selected material to the parameter or said material to be measured, an elongate optical waveguide at least partly immersed in said selected material, and means to measure the transmission of light passed along the optical waveguide, whereby to indicate the value of said parameter.
Where the parameter is temperature, the container is thermally conducting to ensure that said selected material is at substantially the same temperature as said material.
where the parameter is pressure, the container includes provision to allow the said selected material to be subject to the same pressure as said material.
According to a further aspect of the invention, there is provided apparatus for measuring the level of a liquid or fluid powdered material including an elongate optical waveguide along which light is passed by internal reflection, to be immersed vertically in the material, the waveguide having along the length thereof successive inwardly reflecting bands on the surface, with clear bands between the reflective bands, and means to measure the transmission of light passed along the optical waveguide, whereby to indicate the level of the said material in contact with the waveguide.
Various embodiments of the invention are described, by way of example only, with reference to the accompanying drawings, in which: Figure 1 is a section in a vertical central plane of a temperature probe according to the invention; Figure 2 shows part of the probe shown in Figure 1 at enlarged scale; Figure 3 shows part of a pressure probe which is similar to the temperature probe in Figure 2, according to the invention; Figure 4 shows part of a level measurement probe which is similar to the temperature probe of Figure 2, according to the invention; and Figure 5 is a block diagram of a system for using the probes shown in Figures 1 to 4.
In Figure 1 a temperature probe, indicated generally at 10, is immersed in a fluid material 11, of which the temperature is to be measured. lhe probe 10 includes a thermally conducting elongate vessel 12 containing a fluid 13, and especially a liquid, of which the variation of optical refractive index with changes in temperature thereof is known.
An elongate optical transducer or optical waveguide 14 is immersed in the fluid 13 and is of a suitable high quality transparent material such as glass. Ihe cross section of the transducer 14 may be circular but is preferably polygonal, especially of rectangular or square cross section.
Ihe end and side faces of the transducer 14 are preferably polished to optical quality.
A photo-detector 15 is positioned against the bottom face of the transducer 14, to receive all the light emitting therefrom and to produce an electrical signal dependent on the intensity of that light.
Figure 2 shows the transducer 14 in more detail.
Ire upper and lower lengths 16,17 of all the side faces of the transducer 14 and also the upper end face 18 are all provided with a mirror-like reflective coating, such as deposited silver or aluminium. The faces between the lengths 16,17 are left clear. An optical prism 19 is optically connected with one side face of the transducer by means of a cement or liquid layer 20 having substantially the same refractive index as the transducer 14 and prism 19. There is no reflective coating in the region of the layer 20, so that light 21 entering in the direction shown, will pass through the prism 19, the layer 20 and into the transducer 14, where it is reflected downwardly by the reflective coating.
On reaching the transducer faces which are devoid of reflective coating, the light will be partly reflected within the transducer and partly transmitted into the fluid 13. The ratio of the intensity of the reflected to the transmitted light depends on the refractive indices of the material of the transducer 14 and of the fluid 13. thus, the magnitude of the electrical signal from the photo-detector 15 will also depend on the refractive indices. More importantly, variations in the refractive index of the fluid 13 due to variations in a parameter thereof such as temperature or pressure, will produce a corresponding variation in the electrical signal.
Figures 1 and 2 show how the probe 10 can be used to measure temperature of the fluid 11 as a consequence of the changes in refractive index of the fluid 13 with temperature.
Figure 5 shows how the probe 10 is cpnnected optically and electrically. A light source, which is preferably a laser 22, emits light to a beam splitter 23, from which part of the beam is fed back through a loop comprising a photo-detector compensator 24 and a line 25 to the laser 22, to stabilize and regulate the light output thereof.
The remaining light from the beam splitter 23 enters the transducer of the probe 10, as described above.
The probe 10 emits an electrical signal from the photo-detector 15 along a line 26 to processing hardware 27 and hence to a display 28, which displays the temperature of the fluid 11.
Figure 3 shows a probe used to sense a different parameter of the fluid 11, in this case the pressure thereof, which is known to change the refractive index of certain fluids 13, which fluids are chosen appropriately to the application.
A transducer 14 is provided, as in Figure 2, but changes of refractive index due to temperature are compensated by an almost identical temperature probe.as in Figure 1, or other temperature measurement device thermally bonded to transducer 14. The transducer 14a is fed through a prism 19a with light from the laser 22. The signal from transducer 14a (carrying indication of temperature) is sent to the processing hardware 27, to compensate for the effect of temperature changes. If the refractive index of the material 13 is changed by changes of temperature and pressure, one of these parameters can be held constant and the probe 10 used to measure the other parameter. If temperature cannot be held constant, the embodiment of Figure 3 is used.
Figure 4 shows a level measurement probe which can be used to measure the level of a liquid, or possibly a powdered solid, in which the probe is partly immersed. In this embodiment of the invention, a transducer 14b is fed with light from the laser 22 through a prism 19b. However, a succession of short bands of reflective coating 29 are provided, with intermediate clear bands 30. The lengths and spacing of the bands 29,30 are chosen to provide the required resolution of the particular application and may be equi-spaced or change progressively to provide a non-linear output.
Light emerging from the bottom of the transducer 14b impinges on a photo-transducer 15, as before, and the display 27 shows the height of the liquid or powder material up the transducer 14b, which in this embodiment has no surrounding vessel 12 or fluid 13.
As the level of the material being measured rises up the transducer 14b, it absorbs more light through each clear band 30 which it reaches. Thus, the display 28 shows the changing level of the material up the transducer 14b.
Except for the embodiment of Figure 4, the invention is applicable to measuring suitable parameters of fluid 11 which could be solid, liquid, vapour or gaseous.
In addition to the use of a polygonal or flat-sided cross-section for the transducer or optical waveguide described in the embodiments above, it has been found that a polygonal or flat-sided cross-section is advantageous in transducers or optical waveguides of the optical fibre type.
This is especially so where the normal cladding of the optical fibre is removed from the core thereof, for use in measuring the refractive index of material in which the optical fibre is immersed.
Parameters other than temperature, pressure or level can be measured, such as, for example the concentration of a constituent which causes changes in the refractive index of the material. One such parameter is the glucose concentration in blood.

Claims (6)

CLAIMS:
1. Apparatus for measuring a parameter of a test material through changes in the refractive index thereof produced by or related to changes in said parameter, including an elongate optical waveguide along which light is passed by internal reflection, the waveguide having at least one portion in optical contact with said material and in which the transverse cross section of the said portion has a straight side.
2. Apparatus according to claim 1, wherein the cross-section of said portion is polygonal.
3. Apparatus according to claim 2, wherein said polygonal cross-section is rectangular or square.
4. Apparatus according to any of claims 1 to 3, which further comprises a container holding a quantity of selected material having known variation of refractive index thereof with changes in said parameter, means for subjecting the selected material to the parameter or said material to be measured, at least said portion of said waveguide being immersed in said selected material, said apparatus also including means to measure the transmission of light passed along the optical waveguide, whereby to indicate the value of said parameter.
5. Apparatus according to claim 4, wherein said parameter is temperature and said container is thermally conducting.
6. Apparatus according to claim 4, wherein said parameter is pressure and said container includes means to ensure that said selected material is subject to substantially the same pressure as said test material.
GB8820537A 1988-08-31 1988-08-31 Parameter measurement using refractive index change Withdrawn GB2223841A (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
GB8820537A GB2223841A (en) 1988-08-31 1988-08-31 Parameter measurement using refractive index change
PCT/GB1989/001012 WO1990002322A1 (en) 1988-08-31 1989-08-31 Parameter measurement using refractive index change
AU41914/89A AU4191489A (en) 1988-08-31 1989-08-31 Parameter measurement using refractive index change

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
GB8820537A GB2223841A (en) 1988-08-31 1988-08-31 Parameter measurement using refractive index change

Publications (2)

Publication Number Publication Date
GB8820537D0 GB8820537D0 (en) 1988-09-28
GB2223841A true GB2223841A (en) 1990-04-18

Family

ID=10642924

Family Applications (1)

Application Number Title Priority Date Filing Date
GB8820537A Withdrawn GB2223841A (en) 1988-08-31 1988-08-31 Parameter measurement using refractive index change

Country Status (3)

Country Link
AU (1) AU4191489A (en)
GB (1) GB2223841A (en)
WO (1) WO1990002322A1 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB9111776D0 (en) * 1991-05-31 1991-07-24 De Beers Ind Diamond Determination of the condition of or change in state of an environment
CN107677341B (en) * 2017-10-30 2023-04-07 吉林大学 Optical fiber interference water level sensing device and method based on air refractive index

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB1116560A (en) * 1966-02-12 1968-06-06 Gullick Ltd Improvements in or relating to apparatus for the determination and/or control of the proportions of the constituents in a fluid mixture of emulsion
US3999857A (en) * 1975-05-29 1976-12-28 Monsanto Research Corporation Refractive index detector
GB1514977A (en) * 1975-12-02 1978-06-21 Standard Telephones Cables Ltd Detecting oil in water
GB1530997A (en) * 1974-11-11 1978-11-01 Monsanto Co Optical analytical method and device
GB1543914A (en) * 1976-02-06 1979-04-11 Monsanto Co Organic vapour detector
EP0074788A2 (en) * 1981-09-10 1983-03-23 The Board Of Trustees Of The Leland Stanford Junior University Fiber coupler temperature tranducer
WO1985003360A2 (en) * 1984-01-20 1985-08-01 Hughes Aircraft Company Fiber optic structure and method for making
GB2173296A (en) * 1985-03-15 1986-10-08 Sharp Kk Optical pressure sensor

Family Cites Families (15)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB1582768A (en) * 1977-08-26 1981-01-14 Standard Telephones Cables Ltd Temperature sensitive optical fibre
US4151747A (en) * 1978-06-21 1979-05-01 Electric Power Research Institute, Inc. Monitoring arrangement utilizing fiber optics
US4201446A (en) * 1978-10-20 1980-05-06 Honeywell Inc. Fiber optic temperature sensor using liquid component fiber
US4203326A (en) * 1979-01-26 1980-05-20 Electric Power Research Institute, Inc. Method and means for improved optical temperature sensor
US4316388A (en) * 1979-02-22 1982-02-23 Westinghouse Electric Corp. Temperature detection using the refractive indices of light guides
SE7903175L (en) * 1979-04-10 1980-10-11 Asea Ab FIBEROPTICAL METDON
DE3045085C2 (en) * 1980-11-29 1986-01-23 Dornier System Gmbh, 7990 Friedrichshafen Temperature sensor
EP0061884A1 (en) * 1981-03-30 1982-10-06 Imperial Chemical Industries Plc Optical fibre sensor
AU557816B2 (en) * 1981-09-18 1987-01-08 Prutec Ltd. Method for the determination of species in solution with an optical wave-guide
IT1158799B (en) * 1982-11-18 1987-02-25 Consiglio Nazionale Ricerche OPTICAL FIBER THERMOMETER
DE3321203A1 (en) * 1983-06-11 1984-12-13 Phönix Armaturen-Werke Bregel GmbH, 6000 Frankfurt REFRACTOMETER
US4756627A (en) * 1984-08-17 1988-07-12 Sperry Corporation Optical temperature sensor using photoelastic waveguides
US4689483A (en) * 1985-04-25 1987-08-25 Advanced Fiberoptic Technologies Corporation Fiber optical temperature measuring apparatus
GB2186073B (en) * 1986-02-03 1989-10-25 Spectran Corp Fiber optic pressure sensor
AU579041B2 (en) * 1986-05-09 1988-11-10 Thomas & Betts Corporation Method of and apparatus for fiber optic sensing

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB1116560A (en) * 1966-02-12 1968-06-06 Gullick Ltd Improvements in or relating to apparatus for the determination and/or control of the proportions of the constituents in a fluid mixture of emulsion
GB1530997A (en) * 1974-11-11 1978-11-01 Monsanto Co Optical analytical method and device
US3999857A (en) * 1975-05-29 1976-12-28 Monsanto Research Corporation Refractive index detector
GB1514977A (en) * 1975-12-02 1978-06-21 Standard Telephones Cables Ltd Detecting oil in water
GB1543914A (en) * 1976-02-06 1979-04-11 Monsanto Co Organic vapour detector
EP0074788A2 (en) * 1981-09-10 1983-03-23 The Board Of Trustees Of The Leland Stanford Junior University Fiber coupler temperature tranducer
WO1985003360A2 (en) * 1984-01-20 1985-08-01 Hughes Aircraft Company Fiber optic structure and method for making
GB2173296A (en) * 1985-03-15 1986-10-08 Sharp Kk Optical pressure sensor

Also Published As

Publication number Publication date
WO1990002322A1 (en) 1990-03-08
GB8820537D0 (en) 1988-09-28
AU4191489A (en) 1990-03-23

Similar Documents

Publication Publication Date Title
US5004913A (en) Remote measurement of physical variables with fiber optic systems - methods, materials and devices
US4745293A (en) Method and apparatus for optically measuring fluid levels
US4994682A (en) Fiber optic continuous liquid level sensor
Villatoro et al. High resolution refractive index sensing with cladded multimode tapered optical fibre
US4870292A (en) Fibre optic sensor for liquid level and other parameters
US5164608A (en) Plural wavelength fiber optic liquid level sensor for multiple liquids
US4699511A (en) Refraction sensor
DE68920138D1 (en) SENSOR FOR THE OPTICAL FIBER BREAKING INDEX USING A METAL COATING.
KR940004880B1 (en) Fiber optic liquid leak detector
US5422714A (en) Device for comparing the refractive indices of an optical immersion liquid and a reference glass
KR940003737B1 (en) Fibre optic liquid level gauge
US6795598B1 (en) Liquid-level sensor having multiple solid optical conductors with surface discontinuities
US4806013A (en) Refractometer for fluids
GB2223841A (en) Parameter measurement using refractive index change
Borsboom et al. Fiber-optic scattering monitor for use with bulk opaque material
SU922538A1 (en) Device for remote measuring of temperature
RU2506568C2 (en) Device to measure index of refraction
JP3071645B2 (en) Refractive index sensor
US5335057A (en) Measuring geometry of optical fibre coatings with transverse incident beams
US5110208A (en) Measurement of average density and relative volumes in a dispersed two-phase fluid
Bobb et al. An optical fiber refractometer
CN212780378U (en) Liquid surface tension coefficient measuring system based on fiber bragg grating
JPH0652237B2 (en) Fluid refractometer and fluid density meter using the same
RU2014572C1 (en) Discrete optical level meter
JPS57194324A (en) Optical temperature measuring device

Legal Events

Date Code Title Description
WAP Application withdrawn, taken to be withdrawn or refused ** after publication under section 16(1)