WO2002073271A1 - Actuator device - Google Patents

Actuator device Download PDF

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Publication number
WO2002073271A1
WO2002073271A1 PCT/SE2002/000431 SE0200431W WO02073271A1 WO 2002073271 A1 WO2002073271 A1 WO 2002073271A1 SE 0200431 W SE0200431 W SE 0200431W WO 02073271 A1 WO02073271 A1 WO 02073271A1
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WO
WIPO (PCT)
Prior art keywords
fibre
actuator
arrangement
optical fibre
sensor
Prior art date
Application number
PCT/SE2002/000431
Other languages
French (fr)
Inventor
Mikael Bergman
Bengt Sahlgren
Original Assignee
Proximion Fiber Optics 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 Proximion Fiber Optics Ab filed Critical Proximion Fiber Optics Ab
Publication of WO2002073271A1 publication Critical patent/WO2002073271A1/en

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Classifications

    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/11Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on acousto-optical elements, e.g. using variable diffraction by sound or like mechanical waves
    • G02F1/125Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on acousto-optical elements, e.g. using variable diffraction by sound or like mechanical waves in an optical waveguide structure
    • 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
    • G01D5/32Mechanical 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 with attenuation or whole or partial obturation of beams of light
    • G01D5/34Mechanical 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 with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
    • G01D5/353Mechanical 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 with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre
    • G01D5/35306Mechanical 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 with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using an interferometer arrangement
    • G01D5/35309Mechanical 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 with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using an interferometer arrangement using multiple waves interferometer
    • G01D5/35316Mechanical 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 with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using an interferometer arrangement using multiple waves interferometer using a Bragg gratings
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/011Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  in optical waveguides, not otherwise provided for in this subclass
    • G02F1/0115Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  in optical waveguides, not otherwise provided for in this subclass in optical fibres
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/02Optical fibres with cladding with or without a coating
    • G02B6/02057Optical fibres with cladding with or without a coating comprising gratings
    • G02B6/02076Refractive index modulation gratings, e.g. Bragg gratings
    • G02B6/02195Refractive index modulation gratings, e.g. Bragg gratings characterised by means for tuning the grating
    • G02B6/022Refractive index modulation gratings, e.g. Bragg gratings characterised by means for tuning the grating using mechanical stress, e.g. tuning by compression or elongation, special geometrical shapes such as "dog-bone" or taper
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/36Mechanical coupling means
    • G02B6/3628Mechanical coupling means for mounting fibres to supporting carriers
    • G02B6/3632Mechanical coupling means for mounting fibres to supporting carriers characterised by the cross-sectional shape of the mechanical coupling means
    • G02B6/3644Mechanical coupling means for mounting fibres to supporting carriers characterised by the cross-sectional shape of the mechanical coupling means the coupling means being through-holes or wall apertures
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/42Coupling light guides with opto-electronic elements
    • G02B6/4201Packages, e.g. shape, construction, internal or external details
    • G02B6/4219Mechanical fixtures for holding or positioning the elements relative to each other in the couplings; Alignment methods for the elements, e.g. measuring or observing methods especially used therefor
    • G02B6/422Active alignment, i.e. moving the elements in response to the detected degree of coupling or position of the elements
    • G02B6/4226Positioning means for moving the elements into alignment, e.g. alignment screws, deformation of the mount
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F1/00Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
    • G02F1/01Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour 
    • G02F1/0128Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on electro-mechanical, magneto-mechanical, elasto-optic effects
    • G02F1/0131Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on electro-mechanical, magneto-mechanical, elasto-optic effects based on photo-elastic effects, e.g. mechanically induced birefringence
    • G02F1/0134Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour  based on electro-mechanical, magneto-mechanical, elasto-optic effects based on photo-elastic effects, e.g. mechanically induced birefringence in optical waveguides
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F2201/00Constructional arrangements not provided for in groups G02F1/00 - G02F7/00
    • G02F2201/02Constructional arrangements not provided for in groups G02F1/00 - G02F7/00 fibre
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
    • G02F2201/00Constructional arrangements not provided for in groups G02F1/00 - G02F7/00
    • G02F2201/30Constructional arrangements not provided for in groups G02F1/00 - G02F7/00 grating
    • G02F2201/307Reflective grating, i.e. Bragg grating

Definitions

  • the present invention relates to acoustic actuators and acoustic sensors, and more particularly to acoustic actuators and sensors arranged to send and detect longitudinal displacement pulses in an optical fibre.
  • the actuators and sensors according to the invention can be employed in a set-up for sending longitudinal displacement pulses along a length of optical fibre between a first reflection point and a second reflection point.
  • an acoustic wave was coupled into an optical fibre by a tapered horn made from fused silica.
  • the horn was tapered in diameter from 3 mm at a first end to 125 ⁇ m at a second end, over a length of 12 cm.
  • a planar piezo-electric transducer was bonded to the first end surface of the silica horn, in order to launch an acoustic wave into the horn.
  • the second end of the horn was fusion-spliced to an end of the optical fibre. Consequently, a longitudinal displacement excited by the piezo-electric transducer was transferred into the optical fibre through said silica horn.
  • the optical fibre must be terminated at the transducer. Consequently, the above-described arrangement does not allow light to propagate from one side of the transducer to the other side .
  • the present invention has several further advanta- geous features, which will be apparent from the detailed description of some preferred embodiments presented below.
  • a longitudinal displacement pulse, or wave can be excited in an optical fibre by quickly moving the fibre at one point even when the fibre is not pre-strained.
  • the inertia of the fibre itself is sufficient for a displacement pulse to be excited by said quick movement of the fibre.
  • longitudinal displacement wave it is meant a compression/elongation propagating along the fibre.
  • a wave or pulse is referred to as a longitudinal acoustic pulse.
  • the present invention provides an actuator arrangement for exciting a longitudinal displace- ment wave, or pulse, in an optical fibre.
  • the arrangement comprises a washer element, or a collar, with which the optical fibre is engaged.
  • the arrangement comprises a piezo member, which is responsive to an applied voltage to displace said washer element with respect to a (comparatively heavy) bracket .
  • the present invention provides a sensor arrangement for sensing longitudinal displacements in an optical fibre.
  • the washer element is not present. Instead of using a washer element, the fibre rests directly onto the piezo member. In such a case, it is preferred to have the fibre pre-strained towards the piezo member by a pulling force.
  • the actuators and sensors according to the present invention can advantageously be employed in an arrangement, or a set-up, for sending a longitudinal displacement pulse through a length of optical fibre.
  • the longitudinal displacement pulse is repeatedly reflected back and forth between two reflection points.
  • the arrangement comprises an actuator arrangement and a sensor arrangement .
  • the actuator arrangement is adapted to actuate and amplify the longitu- dinal displacement pulse
  • the sensor arrangement is adapted to directly or indirectly measure the timing of said pulse in order to provide actuation of the actuator arrangement resonantly with the pulse reflected back and forth between said reflection points.
  • One advantage of the inventive set-up is that a longitudinal displacement pulse can be repeatedly sent along a length of optical fibre without terminating the light guiding path in the fibre.
  • the sensor arrangement is operative to provide an output signal indicative of the amplitude of the displacement pulse propagating between the two re- flection points.
  • Feedback is provided from the sensor arrangement to the actuator arrangement, and actuation of said actuator is adjusted so that the amplitude of the longitudinal displacement pulse, as detected by the sen- sor arrangement, is maximised.
  • Maximum amplitude of the displacement pulse is obtained when the actuator is operated resonantly with the displacement pulse, i.e. when the actuator arrangement is actuated at the same instant as the longitudinal pulse passes said actuator. There- fore, maximising of the pulse amplitude is a sufficient means for operating the actuator resonantly with the longitudinal displacement pulse.
  • the timing of the displacement pulses is measured, and the time of passage be- tween the two reflection points is determined. Feedback is then provided to the actuator arrangement in order to actuate said actuator arrangement at the time when the displacement pulse passes said actuator.
  • the present invention provides a method for repeatedly sending longitudinal displacement waves, or pulses, along a length of optical fibre between a first reflection point and a second reflection point. It is envisioned that the present invention will have its primary field of use in connection with systems in which the reflective properties of fibre Bragg gratings are altered by means of longitudinal displacement waves, or pulses. Such a system is disclosed in the Swedish patent application number 0002415-8, which is incorporated herein by reference.
  • Fig. 1 schematically shows a first embodiment of the present invention
  • Fig. 2 schematically shows a piezo member comprised of two semi-circular parts
  • FIG. 3 schematically shows a second embodiment of the present invention
  • Fig. 4 schematically shows a third embodiment of the present invention.
  • Fig. 5 schematically shows a set-up for sending longitudinal displacement pulses, or waves, into a length of optical fibre.
  • a first preferred embodiment of an actuator arrangement according to the present invention is schematically shown in figure 1.
  • FIG 1 a cross-section of an actuator arrangement 10 is shown.
  • the arrangement comprises a bracket 11, or support, which is comparatively heavy with respect to other parts of the arrangement.
  • the arrangement comprises a washer element 12 and a piezo member 13.
  • the piezo member 13 is arranged between the bracket 11 and the washer element 12, and is operative, responsive to an applied voltage, to displace said washer element 12 with respect to the bracket 11, i.e. to change the separation of the washer from the bracket.
  • a predefined portion of an optical fibre 14 is engaged with the washer element 12 in such a way that said portion of the optical fibre follows any movement of the washer element.
  • the fibre 14 is engaged with the washer element 12 by means of a girdle 15, or bulb, on the fibre, said girdle being jammed to a passage in the washer element.
  • the fibre can be attached to or engaged with the washer in any suitable way, as long as the requirement that the en- Lo LO IV) > H 1 H
  • a piezo-electric material can alter its dimensions responsive to an applied voltage.
  • a change of the dimensions of a piezo-electric material can produce an output voltage if electrical connections are applied appropriately.
  • the piezo mem- ber of the actuator arrangement is electrically connected to an external voltage supply.
  • bracket 11 due to the relatively large inertia of the bracket 11, a sudden change of the separation between the bracket 11 and the washer element 12 caused by the piezo member 13, causes a displacement only of the washer element 12 and of the portion of the fibre engaged therewith. Furthermore, the bracket 11 may be firmly attached to an external housing.
  • tion where the set-up of figure 5 is employed is when longitudinal displacement waves, or pulses, are used in order to alter the reflectivity of a fibre Bragg grating.
  • a fibre Bragg grating that reflects light in an unper- turbed state can be made to pass, temporarily and for a narrow wavelength range only, light when a localised and temporary compression and/or elongation is present in the grating.
  • the set-up shown in figure 5 comprises a bracket 11, an actuator arrangement 50 and a sensor arrangement 51, the bracket 11 acting as a common support for said actuator 50 and said sensor 51. Furthermore, the set-up includes a length of optical fibre 52 having a fibre Bragg grating incorporated in its core. Typically, the Bragg grating is a chirped grating constituting, in an unperturbed state, a continuous broadband reflector. Said length of fibre 52 is engaged with a washer element of the actuator arrangement 50 and with a washer element of the sensor arrangement 51, for exciting longitudinal dis- placement waves in the fibre and for sensing longitudinal displacement waves in the fibre, respectively. The length of fibre 52 comprising the Bragg grating is arranged between said actuator 50 and said sensor 51.
  • An input end of said length of fibre is connected, by means of a first fibre connector 61, to a first piece of standard fibre 53.
  • said first piece of standard fibre 53 is provided with an input fibre connector 54 to which an external input fibre is to be connected.
  • an output end of said length of fibre is con- nected, by means of a second fibre connector 62, to a second piece of standard fibre 55.
  • said second piece of standard fibre is provided with an output fibre connector 56 to which an external output fibre is to be connected. It is to be noted that there is a continuous light path through the optical fibre between said input fibre connector 54 and said output fibre connector 56. co ) to to ⁇ 1 ⁇ >
  • the amplitude of the longitudinal displacement pulse is monitored continuously during operation, and the output of the monitoring is utilised for adjust- ing the actuator so that the actuator is actuated at a rate that gives maximum amplitude of the displacement pulse propagating in the length of fibre, i.e. at a rate that is in concert with the roundtrip rate of the displacement pulse between the two reflectors.

Abstract

The present invention relates to an actuator arrangement for exciting longitudinal displacement pulses, or waves, in an optical fibre. The arrangement comprises a bracket, a washer element, a piezo member arranged between the bracket and the washer element, and an optical fibre that is engaged with an extending through a passage in the washer element. The piezo member is operative, responsive to an applied voltage, to displace the washer element and the fibre engaged therewith, in the longitudinal direction of the fibre, with respect to the bracket. Thereby, a longitudinal displacement pulse may be excited in the optical fibre. The actuator arrangement may also operate as a sensor for sensing longitudinal displacements in optical fibres. A set-up and a method for repeatedly sending longitudinal displacement pulses through a length of optical fibre is also disclosed.

Description

ACTUATOR DEVICE
Technical field
The present invention relates to acoustic actuators and acoustic sensors, and more particularly to acoustic actuators and sensors arranged to send and detect longitudinal displacement pulses in an optical fibre. The actuators and sensors according to the invention can be employed in a set-up for sending longitudinal displacement pulses along a length of optical fibre between a first reflection point and a second reflection point.
Technical background
It is known in the prior art to alter the reflectivity of fibre Bragg gratings in optical fibres by means of longitudinal acoustic waves, i.e. longitudinal displace- ment waves.
One way of coupling an acoustic wave into an optical fibre is presented in the article "100% efficient narrowband acoustooptic tunable reflector using fiber Bragg grating", Liu et al . , Journal of Lightwave Technology, Vol. 16, No. 11, November 1998. According to said journal article, an acoustic wave was coupled into an optical fibre by a tapered horn made from fused silica. The horn was tapered in diameter from 3 mm at a first end to 125 μm at a second end, over a length of 12 cm. A planar piezo-electric transducer was bonded to the first end surface of the silica horn, in order to launch an acoustic wave into the horn. The second end of the horn was fusion-spliced to an end of the optical fibre. Consequently, a longitudinal displacement excited by the piezo-electric transducer was transferred into the optical fibre through said silica horn.
However, the optical fibre must be terminated at the transducer. Consequently, the above-described arrangement does not allow light to propagate from one side of the transducer to the other side .
In many cases, it is desirable to launch acoustic waves into an optical fibre without terminating the light propagation path. This, however, not being allowed by the arrangement described above. Thus, there is a need for new and improved arrangements for sending longitudinal acoustic waves, or longitudinal displacement waves or pulses, into an optical fibre.
Summary of the invention
It is an object of the present invention to provide a new and improved arrangement for sending longitudinal displacement waves, or pulses, into an optical fibre and the like, by which arrangement at least the above- identified problem of the prior art is eliminated. This object is achieved by an arrangement according to the accompanying claims.
The present invention has several further advanta- geous features, which will be apparent from the detailed description of some preferred embodiments presented below.
Surprisingly, it has been found that a longitudinal displacement pulse, or wave, can be excited in an optical fibre by quickly moving the fibre at one point even when the fibre is not pre-strained. The inertia of the fibre itself is sufficient for a displacement pulse to be excited by said quick movement of the fibre.
By longitudinal displacement wave, it is meant a compression/elongation propagating along the fibre. Sometimes, such a wave or pulse is referred to as a longitudinal acoustic pulse.
In one aspect, the present invention provides an actuator arrangement for exciting a longitudinal displace- ment wave, or pulse, in an optical fibre. The arrangement comprises a washer element, or a collar, with which the optical fibre is engaged. Furthermore, the arrangement comprises a piezo member, which is responsive to an applied voltage to displace said washer element with respect to a (comparatively heavy) bracket . By virtue of the fibre being engaged with said washer element, said displacement is transferred to the engaged portion of the fibre and propagated along the fibre.
In another aspect, the present invention provides a sensor arrangement for sensing longitudinal displacements in an optical fibre. In some embodiments of the actuator or sensor arrangement above, the washer element is not present. Instead of using a washer element, the fibre rests directly onto the piezo member. In such a case, it is preferred to have the fibre pre-strained towards the piezo member by a pulling force.
The actuators and sensors according to the present invention can advantageously be employed in an arrangement, or a set-up, for sending a longitudinal displacement pulse through a length of optical fibre. In said length of optical fibre, the longitudinal displacement pulse is repeatedly reflected back and forth between two reflection points. The arrangement comprises an actuator arrangement and a sensor arrangement . The actuator arrangement is adapted to actuate and amplify the longitu- dinal displacement pulse, and the sensor arrangement is adapted to directly or indirectly measure the timing of said pulse in order to provide actuation of the actuator arrangement resonantly with the pulse reflected back and forth between said reflection points. One advantage of the inventive set-up is that a longitudinal displacement pulse can be repeatedly sent along a length of optical fibre without terminating the light guiding path in the fibre.
In a preferred mode of operation of the above- described set-up, the sensor arrangement is operative to provide an output signal indicative of the amplitude of the displacement pulse propagating between the two re- flection points. Feedback is provided from the sensor arrangement to the actuator arrangement, and actuation of said actuator is adjusted so that the amplitude of the longitudinal displacement pulse, as detected by the sen- sor arrangement, is maximised. Maximum amplitude of the displacement pulse is obtained when the actuator is operated resonantly with the displacement pulse, i.e. when the actuator arrangement is actuated at the same instant as the longitudinal pulse passes said actuator. There- fore, maximising of the pulse amplitude is a sufficient means for operating the actuator resonantly with the longitudinal displacement pulse.
In another mode of operation, the timing of the displacement pulses is measured, and the time of passage be- tween the two reflection points is determined. Feedback is then provided to the actuator arrangement in order to actuate said actuator arrangement at the time when the displacement pulse passes said actuator.
Furthermore, the present invention provides a method for repeatedly sending longitudinal displacement waves, or pulses, along a length of optical fibre between a first reflection point and a second reflection point. It is envisioned that the present invention will have its primary field of use in connection with systems in which the reflective properties of fibre Bragg gratings are altered by means of longitudinal displacement waves, or pulses. Such a system is disclosed in the Swedish patent application number 0002415-8, which is incorporated herein by reference.
Brief description of the drawings
In the detailed description presented below of some preferred embodiments of the present invention, reference is made to the accompanying drawings, on which: Fig. 1 schematically shows a first embodiment of the present invention;
Fig. 2 schematically shows a piezo member comprised of two semi-circular parts;
Fig. 3 schematically shows a second embodiment of the present invention;
Fig. 4 schematically shows a third embodiment of the present invention; and
Fig. 5 schematically shows a set-up for sending longitudinal displacement pulses, or waves, into a length of optical fibre.
On the drawings, like parts are indicated by like reference numerals.
Detailed description of preferred embodiments
A first preferred embodiment of an actuator arrangement according to the present invention is schematically shown in figure 1.
In figure 1, a cross-section of an actuator arrangement 10 is shown. As will be explained below, the same structural arrangement can also operate as a sensor. The arrangement comprises a bracket 11, or support, which is comparatively heavy with respect to other parts of the arrangement. Further, the arrangement comprises a washer element 12 and a piezo member 13. The piezo member 13 is arranged between the bracket 11 and the washer element 12, and is operative, responsive to an applied voltage, to displace said washer element 12 with respect to the bracket 11, i.e. to change the separation of the washer from the bracket. A predefined portion of an optical fibre 14 is engaged with the washer element 12 in such a way that said portion of the optical fibre follows any movement of the washer element. In the embodiment illustrated in figure 1, the fibre 14 is engaged with the washer element 12 by means of a girdle 15, or bulb, on the fibre, said girdle being jammed to a passage in the washer element. However, it is to be understood that the fibre can be attached to or engaged with the washer in any suitable way, as long as the requirement that the en- Lo LO IV) > H1 H
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the bracket 11 and the piezo member 13, as schematically shown in figure 3.
Although it is preferred to have a washer element resting on the piezo member, and to have the fibre en- gaged with the washer element, it is conceivable to have the fibre itself resting directly on the piezo member. In case the washer element is omitted, it is preferred to have the fibre pre-strained against the piezo member, as will be further described in connection with figure 4. Having described the basic structural features of the actuator arrangement according to the present invention, the operation thereof will now be described in more detail .
It is well known to the man skilled in the art that a piezo-electric material can alter its dimensions responsive to an applied voltage. Likewise, it is well known that a change of the dimensions of a piezo-electric material can produce an output voltage if electrical connections are applied appropriately. Hence, the piezo mem- ber of the actuator arrangement is electrically connected to an external voltage supply. By applying a voltage to the piezo member, its dimensions parallel to the longitudinal dimension of the fibre can be altered. Consequently, the separation between the bracket and the washer element can be altered. It is to be understood that, due to the relatively large inertia of the bracket 11, a sudden change of the separation between the bracket 11 and the washer element 12 caused by the piezo member 13, causes a displacement only of the washer element 12 and of the portion of the fibre engaged therewith. Furthermore, the bracket 11 may be firmly attached to an external housing.
If the change in separation between the bracket and the washer is sufficiently quick, the inertia of the op- tical fibre will, at least to some extent, counteract the displacement. This lead to a longitudinal displacement pulse being excited in the fibre. LO LO t to M
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tion where the set-up of figure 5 is employed is when longitudinal displacement waves, or pulses, are used in order to alter the reflectivity of a fibre Bragg grating. A fibre Bragg grating that reflects light in an unper- turbed state can be made to pass, temporarily and for a narrow wavelength range only, light when a localised and temporary compression and/or elongation is present in the grating.
The set-up shown in figure 5 comprises a bracket 11, an actuator arrangement 50 and a sensor arrangement 51, the bracket 11 acting as a common support for said actuator 50 and said sensor 51. Furthermore, the set-up includes a length of optical fibre 52 having a fibre Bragg grating incorporated in its core. Typically, the Bragg grating is a chirped grating constituting, in an unperturbed state, a continuous broadband reflector. Said length of fibre 52 is engaged with a washer element of the actuator arrangement 50 and with a washer element of the sensor arrangement 51, for exciting longitudinal dis- placement waves in the fibre and for sensing longitudinal displacement waves in the fibre, respectively. The length of fibre 52 comprising the Bragg grating is arranged between said actuator 50 and said sensor 51.
An input end of said length of fibre is connected, by means of a first fibre connector 61, to a first piece of standard fibre 53. In turn, said first piece of standard fibre 53 is provided with an input fibre connector 54 to which an external input fibre is to be connected. Similarly, an output end of said length of fibre is con- nected, by means of a second fibre connector 62, to a second piece of standard fibre 55. In turn, said second piece of standard fibre is provided with an output fibre connector 56 to which an external output fibre is to be connected. It is to be noted that there is a continuous light path through the optical fibre between said input fibre connector 54 and said output fibre connector 56. co ) to to μ1 μ>
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displacement pulse between the reflectors. Any other timing of the actuator would give the displacement pulse lower amplitude. Thus, by tuning the actuation of the actuator arrangement so that the pulse amplitude, as de- tected by the sensor arrangement, is maximised, said actuation will be in resonance with the displacement pulse. Preferably, the amplitude of the longitudinal displacement pulse is monitored continuously during operation, and the output of the monitoring is utilised for adjust- ing the actuator so that the actuator is actuated at a rate that gives maximum amplitude of the displacement pulse propagating in the length of fibre, i.e. at a rate that is in concert with the roundtrip rate of the displacement pulse between the two reflectors. As mentioned above, favourable effects may be achieved by providing the fibre with a bend between the two reflection points (i.e. between the actuator and the sensor) . If the fibre is straight between the reflection points, there is a risk of standing waves building up therein. By providing the fibre with a bend between the reflection points, the risk of standing waves evolving is reduced. However, the propagation of a longitudinal displacement pulse along the length of fibre is virtually unaffected by said bend. Consequently, by providing the length of optical fibre between the actuator 50 and the sensor 51 with a bend, noise due to build-up of standing waves is reduced. The curvature of the bend should, of course, be sufficiently large in order for light not to leak out from the fibre core. The invention has been described above by means of some preferred embodiments, schematically shown on the accompanying drawings. However, it is to be understood that various alterations and modifications are conceivable within the scope of the invention, as defined in the appended claims.

Claims

1. An actuator arrangement for exciting a longitudinal displacement pulse in an optical fibre, comprising a bracket, a piezo member, and an optical fibre extending through a passage in said piezo member, wherein said piezo member is operative, responsive to an applied voltage, to rapidly displace a portion of the fibre, in the longitudinal direction of said fibre, with respect to the bracket, such that a longitudinal displacement pulse is excited in said optical fibre.
2. An actuator arrangement as claimed in claim 1, further comprising a washer element with which the fibre is engaged, the washer element having a passage through which the fibre extends in its longitudinal direction, wherein the piezo member is arranged between the bracket and said washer element, the piezo member being operative, responsive to an applied voltage, to rapidly displace the washer element and the portion of the fibre engaged therewith, in the longitudinal direction of said fibre, with respect to the bracket, such that a longitu- dinal displacement pulse is excited in said optical fibre.
3. An actuator arrangement as claimed in claim 1 or 2, wherein the piezo member comprises two separate parts, each of said parts having the general shape of a semicircular disc.
4. An actuator arrangement as claimed in any one of the claims 1 to 3, wherein the fibre extends through a pas- sage in the bracket, the washer element and the piezo member, respectively.
5. An actuator arrangement as claimed in any one of the preceding claims, wherein the optical fibre is engaged with the washer element by means of a bulb on said fibre being clamped thereto.
6. An actuator arrangement as claimed in any one of the claims 1 to 4, wherein the optical fibre is engaged with the washer element by a pulling force pulling a bulb on said fibre against said washer element.
7. A sensor arrangement for sensing longitudinal displacement pulses in an optical fibre, comprising a bracket, a piezo member, and an optical fibre extending through a passage in said piezo member, wherein said piezo member is operative, responsive to a displacement pulse with respect to said bracket of said fibre in the longitudinal direction thereof, to pro- vide an output voltage indicative of said displacement pulse .
8. A sensor arrangement as claimed in claim 7, further comprising a washer element with which the fibre is en- gaged, the washer element having a passage through which the fibre extends in its longitudinal direction, wherein the piezo member is arranged between the bracket and said washer element, the piezo member being operative, responsive to a displacement pulse of said washer element in the longitudinal direction of said fibre with respect to the bracket, to provide an output voltage indicative of said displacement pulse.
9. A sensor arrangement as claimed in claim 7 or 8, wherein the piezo member comprises two separate parts, each of said parts having the general shape of a semicircular disc.
10. A sensor arrangement as claimed in any one of the claims 7 to 9, wherein the fibre extends through a passage in the bracket, the washer element and the piezo member, respectively.
11. A sensor arrangement as claimed in any one of the claims 7 to 10, wherein the optical fibre is engaged with the washer element by means of a bulb on said fibre being clamped thereto.
12. A sensor arrangement as claimed in any one of the claims 7 to 10, wherein the optical fibre is engaged with the washer element by a pulling force pulling a bulb on said fibre against said washer element .
13. An arrangement for sending a longitudinal displacement pulse along a length of optical fibre between a first reflection point and a second reflection point, the arrangement comprising an actuator operative to excite a longitudinal displacement pulse in said length of fibre; and a sensor for sensing longitudinal displacements in said length of fibre, wherein said first reflection point and said second reflection point are arranged to reflect said pulse excited by said actuator, the actuator further being operative to amplify said pulse as it passes the actuator based on feedback provided by said sensor, said optical fibre being engaged with and extending through a respective passage in said actuator and said sensor.
14. An arrangement as claimed in claim 13 , wherein the actuator constitutes the first reflection point, and the sensor constitutes the second reflection point.
15. An arrangement as claimed in claim 14, further comprising a feedback loop from the sensor to the actuator, a sensor output signal in said feedback loop causing the actuator to amplify the longitudinal displacement pulse at the time when said actuator is reached by a previous displacement pulse, reflected from the sensor.
16. An arrangement as claimed in any one of the claims 13 to 15, wherein the optical fibre is engaged with the actuator and the sensor by means of a bulb on said fibre being clamped to a respective washer element of the actuator and the sensor.
17. An arrangement as claimed in claim 16, wherein the actuator comprises a piezo member operative, responsive to an applied voltage, to displace the washer element and the optical fibre engaged therewith.
18. An arrangement as claimed in claim 17, wherein the piezo member comprises two separate parts, each of said parts having the general shape of a semi-circular disc.
19. An arrangement as claimed in claim 16, wherein the sensor comprises a piezo member operative, responsive to a longitudinal displacement pulse in the optical fibre, to provide an output voltage indicative of the amplitude of said displacement pulse.
20. An arrangement as claimed in claim 19, wherein the piezo member comprises two separate parts, each of said parts having the general shape of a semi-circular disc.
21. An arrangement as claimed in any one of the claims 13 to 20, wherein the optical fibre is provided with a bend between the actuator and the sensor.
22. A method for repeatedly sending longitudinal displacement pulses through a length of optical fibre between a first reflection point and a second reflection point, said length of fibre being engaged with and ex- tending through a respective passage in an actuator and a sensor, the method comprising the steps of: sending, by means of said actuator, a longitudinal displacement pulse into said length of optical fibre; detecting, by means of said sensor, the amplitude of said displacement pulse; and amplifying, by means of said actuator, the displacement pulse in said length of optical fibre at a time when it reaches said actuator, after one or several reflections, the timing being based on feedback from said sen- sor.
23. A method as claimed in claim 22, further comprising the step of adjusting the timing of longitudinal pulses sent into the length of optical fibre, based on the de- tected amplitude of said displacement pulse.
24. A method as claimed in claim 23, wherein the step of adjusting the timing is performed in fine increments until the detected amplitude is maximised.
25. A method as claimed in claim 24, wherein the step of adjusting the timing is performed repeatedly.
26. A method as claimed in any one of the claims 22 to 25, wherein the step of sending a longitudinal pulse into the length of optical fibre is performed by means of an actuator arrangement as defined in any one of the claims 1 to 6.
27. A method as claimed in any one of the claims 22 to 26, wherein the step of detecting the amplitude of the displacement pulse includes detecting said pulse by means of a sensor arrangement as defined in any one of the claims 7 to 12.
PCT/SE2002/000431 2001-03-14 2002-03-11 Actuator device WO2002073271A1 (en)

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SE0100868-9 2001-03-14
SE0100868A SE522291C2 (en) 2001-03-14 2001-03-14 Arrangement and method for sending a longitudinal displacement pulse along an optical fiber

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CN104257363B (en) * 2014-10-23 2017-01-11 山东省科学院激光研究所 FBG (Fiber Bragg Grating) pulse-taking sensor probe and intensive array type optical fiber pulse-taking instrument

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