CN106796125A - Interference determination sensor with differential modulated phase-detection - Google Patents

Interference determination sensor with differential modulated phase-detection Download PDF

Info

Publication number
CN106796125A
CN106796125A CN201580009312.1A CN201580009312A CN106796125A CN 106796125 A CN106796125 A CN 106796125A CN 201580009312 A CN201580009312 A CN 201580009312A CN 106796125 A CN106796125 A CN 106796125A
Authority
CN
China
Prior art keywords
sensor
phase shift
modulator
phase
detector
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.)
Granted
Application number
CN201580009312.1A
Other languages
Chinese (zh)
Other versions
CN106796125B (en
Inventor
顾逊
S.V.马彻塞
K.博内特
A.弗兰克
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.)
Hitachi Energy Co ltd
Hitachi Energy Ltd
Original Assignee
ABB Schweiz AG
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 ABB Schweiz AG filed Critical ABB Schweiz AG
Publication of CN106796125A publication Critical patent/CN106796125A/en
Application granted granted Critical
Publication of CN106796125B publication Critical patent/CN106796125B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

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
    • G01D5/266Mechanical 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 by interferometric 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
    • G01D5/32Mechanical 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
    • 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
    • G01D5/35303Mechanical 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 a reference fibre, e.g. interferometric devices
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R15/00Details of measuring arrangements of the types provided for in groups G01R17/00 - G01R29/00, G01R33/00 - G01R33/26 or G01R35/00
    • G01R15/14Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks
    • G01R15/24Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using light-modulating devices
    • G01R15/241Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using light-modulating devices using electro-optical modulators, e.g. electro-absorption
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/02Measuring direction or magnitude of magnetic fields or magnetic flux
    • G01R33/032Measuring direction or magnitude of magnetic fields or magnetic flux using magneto-optic devices, e.g. Faraday or Cotton-Mouton effect
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/02Measuring direction or magnitude of magnetic fields or magnetic flux
    • G01R33/032Measuring direction or magnitude of magnetic fields or magnetic flux using magneto-optic devices, e.g. Faraday or Cotton-Mouton effect
    • G01R33/0327Measuring direction or magnitude of magnetic fields or magnetic flux using magneto-optic devices, e.g. Faraday or Cotton-Mouton effect with application of magnetostriction

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • Gyroscopes (AREA)

Abstract

A kind of sensor is provided, it has:Sensing element (8), thus measurand cause the relative phase shift between two ripples;Phase-modulator (5), relative phase shift is added to by modulation;At least two detectors (10 1,10 2), wherein the first detector (10 1) does not include in response to relative phase shift and interference signal is detected such as the relative phase shift as caused by measurand, and wherein the second detector (10 2) includes detecting interference signal such as the relative phase shift as caused by measurand in response to relative phase shift;And also including signal processing unit (11), its suitable analysis two detects interference signal, and draws measurand value therefrom.

Description

Interference determination sensor with differential modulated phase-detection
Technical field
The present invention relates to the interference determination sensor using phase modulation detection scheme.
Background technology
US 3707329 describes a kind of equipment for analyzing the light beam modulated by amount to be measured.It includes machinery Chopper, its amplitude that light beam was modulated before light beam enters electro-optical sensor.
DE 19544778 describes a kind of current sensor, and wherein the two of the sensing optical fiber of different length section twine around conductor Around(would).
It is known by the sensor of the interference between two ripples, typically two orthogonal polarization modes of ripple, and (referring to bibliography [1]-[7]) in for large-scale technical field.The detector signal of these sensors and two ripples it Between relative phase shiftCosine it is related.Phase shift can be detected using such as polarimetry scheme.This sensor typically will Seek multiple detector channels (such as two cross-polarizations determine the reference channel of passage and measurement total optical power).In order to meet one High accuracy requirement in a little applications, such as DC Electro-optical voltages sensing, it is necessary to extremely good relatively steady between the multiple passages of holding Qualitative (protection precision ~ 1-5% opposing channels stability), this is serious practical challenge.
Interference determination sensor also can detect (MPD) skill using the phase modulation as described in such as bibliography [8] Art, builds according to open loop and closed loop configurations.MPD technologies are general to be realized in " nonreciprocal phase-modulation " scheme, and is led to It is usually used in fibre optic gyroscope (FOG) and fibre optic current sensor (FOCS) ([9,10]).Jointly owned patent US 7911196 [11] descriptions it is a kind of according to combine Voltage sensing element (or some this class components), 45 ° of Faraday rotators with And the voltage sensor of the reflection configuration of MPD modulation and detection electronic device.Similar system with landscape configuration voltage cell Can see [12].
But polarimetry optical phase measurement usually requires that the comparing of the luminous power measured by multiple detectors, In MPD, fast phase modulation is added in phase shift to be measured, and only need a detector come measure response wave shape and from Wherein calculate phase shift.MPD phase shifts calculate unrelated with the absolute level of measurement power, and therefore to resulting from low-frequency vibration and ring (it can change the optical power fluctuation of border disturbance between different detectors, but can not change the shape of the waveform of detectors measure Shape (as long as disturbance is much smaller than modulating frequency)) it is inherently immune(immune).
So far, the design of actual MPD sensors uses " nonreciprocal phase-modulation " principle.This kind of sensor can mainly be drawn It is divided into two classes:Sagnac interferometer configuration and reflection configuration.Optical design is interactive, it is meant that must be offset in circuit Propagation during all intrinsic phase shift accumulated.But, the measurand in sensing element causes phase shift and by modulator institute The phase-modulation forced is noninteractive and is added up to.Therefore, interference ripple before it reaches the detectors must be in phase negative side Upwards twice by phase-modulator and any interconnection fabric.Single mode (polarization keep (PM)) optical fiber is needed to be to and from determining The optical phase modulator transmission ripple of adopted phase shift (and polarization).For signal transacting, closed loop and open loop policy are developed, with from Measured waveform extracts measurand and causes phase shift, see, for example, [8].
The principle of interaction design has been essential in all actual MPD sensors, because phase-modulator and PM Intrinsic phase shift in both optical fiber is extremely sensitive to temperature or stress disturbance.Therefore, in the feelings without interaction optics circuit system Under condition, simple MPD equipment will not reliably work in real world environments, because measurement phase shift will be held by environmental perturbation Continuous disturbance.On the other hand, using interaction design, MPD sensors are verified to obtain the outstanding phase with notable DC stability Measurement accuracy.
Realize that the interactive optical design of all -fiber device, such as FOG or FOCS is relatively simple, because in this kind of device, Optical fiber is in itself that high coupling efficiency of the sensing between medium, and various optical fiber components can be spliced by standard(splicing) It is reliably achieved.But, it is not optical fiber but the sensor of such as block elements for wherein sensing element, with optical fiber coupling The interactive optical design for closing optical phase modulator is quite difficult to.That because, by bulk optical sensing element it Afterwards, light must be coupled back in single-mode fiber (same fibre in reflection configuration before sensing element), and for It is alone sizable technological challenge that high efficiency and reliability is done like that.
According to above, it will thus provide one kind need not be from sensing element, (it has using differential modulated Phase Detecting Device Body can be bulk optical sensing element) regard the present invention as optically coupling to the interference determination sensor in single-mode fiber or waveguide Purpose.
The content of the invention
Therefore, according to the first aspect of the present invention, there is provided one kind interference determination sensor, it has:Sensing element, thus Measurand causes the relative phase shift between two ripples;Phase-modulator, relative phase shift is added to by modulation;At least two detections Device, wherein the first detector response does not cause relative phase shift and detects interference signal in relative phase shift comprising measurand, and And wherein the second detector response causes relative phase shift and detects interference signal in relative phase shift comprising measurand.Can compare Two signals, to draw measurand value therefrom.
The physical significance by verbatim means to be included in all of room and time propagation term " ripple " herein The vibration of type.Ripple can have narrow or wide range content, can be permanent or be restricted in duration, Yi Jike By the generation of source or from multiple source synthesis.The property of ripple generally can be mechanical (sound), electromagnetism (light), or have Any other type.In being described below, the present invention described as an example using light wave.Two interference wave energy are enough such as light Two orthogonal linears or circular polarisation mode of ripple.
In preferred embodiment in this aspect of the invention, after being modulated by phase-modulator, light wave is entering By beam splitter before sensing element, and two groups of polarizers and detector respectively respectively measurement sensing element before and after do Disturb signal.Phase shift is independently retrieved with two measured waveforms, and their difference produces the phase shift inside sensing medium, and it is then It is converted into measurand value.
Therefore, using the present invention, sensor can be with the reduction to the phase shift variations in the wave path outside sensing element Sensitivity builds, while do not require that ripple returns to phase-modulator along same paths.
In order to keep the appropriate coherence high between interference ripple at detector, group postpones biasing element and is preferably able to It is introduced into wave path, so that the intrinsic relative group before and after at least part of compensation sensing element between two ripples postpones.
Group delay compensation can determine that interference contrast value or any related or equivalent metric enter by from interference signal One step strengthens.Interference contrast additionally be able to for provide cycle information (its help from measurement phase shift in remove cycle ambiguousness, And thus extend clear and definite measurement range), or as surround sensor birefringence element at least some of control environment Monitoring signals.
Advantageously, the modulation as caused by phase-modulator is unrelated with measurand.In addition, signal processing unit be adapted to from Modulate to determine the relative phase shift between two ripples as caused by phase-modulator.Specifically, modulation has and is not present in At least one spectral component with given frequency in measurand, and signal processing unit is adapted to determine using given frequency Relative phase shift.
For according to voltage of the invention or electric field measurement, sensing element can include electro-optic crystal, crystallization electric light fibre, pole Change optical fiber or be attached to the optical fiber or Bulk optical material of piezoelectric element.For according to power of the invention or strain measurement, sense Surveying element can include optical fiber or Bulk optical material.For according to optical magnetic field sensors of the invention or current sensor, Sensing element can include optical fiber or waveguide, and it includes professional low birefringent fiber, flint glass optical fiber or spin high birefringence Optical fiber, block magneto-optic memory technique (such as yttrium iron garnet crystal or fused silica glass block) are attached to magnetostriction element Optical fiber, waveguide or Bulk optical material or its combination.
Sensor is special as the sensor for DC signals and more particularly for D/C voltage or electric field measurement Preferably, especially for medium-pressure or high pressure application.But, it can also be potentially applied to fibre optic current sensor, rotation Sensor or other MPD sensors.
It is particularly suitable for the sensor with block sensing element.
Be described below be described in more detail in accompanying drawing it is of the invention above and other aspect have in addition together with of the invention Sharp embodiment and application.
Brief description of the drawings
Fig. 1 is illustrated according to the first example of the invention;
Fig. 2A and Fig. 2 B are shown with the example of the invention of relative group delay compensation;And
Fig. 3 is illustrated according to the example of the invention of reflection configuration.
Specific embodiment
According to Basic Differential MPD sensors example of the invention figure 1 illustrates.Light source 1 generates light wave, and it is via single mode Optical fiber is directed to fibre optic polarizer 2.By 45 ° of fibre-optical splices(splice)4 and in two axles of PM optical fiber 3 carry Polarization light output passes to optical fiber collimator 6 by optical phase modulator 5, and wherein light is coupled from PM optical fiber 3.It is free of birefringence Beam splitter 7 is located between collimator and sensing element 8.By a branch of the separated light output of beam splitter 7 by first piece Shape linear polarization 9-1, and detected by the first photoelectric detector 10-1.Another branch of light output by sensing element 8, Second block linear polarization 9-2, and detected by the second photoelectric detector 10-2.Two detectors 10-1,10-2's is defeated Go out signal and be imported into signal processing unit 11.The optical axis for sensing medium 8 abreast aligns, and block linear polarization 9-1, The axle that the axle of 9-2 snaps to PM optical fiber 3 (it is connected to phase-modulator 5) with 45 °.Optical phase modulator can be Integrated Light Learn LiNbO3Birefringent phase modulator [8,10] has 90 ° of PM light in one of branch as described in bibliography [9] The Y type modulators of fine joint.The phase that another part is made up of the PZT (piezoelectric transducer) with the optical fiber attached with it Modulator [9].
Be added to phase-modulation on the relative phase shift between two interference ripples by phase-modulator 5, and signal transacting list Unit performs independent MPD signal transactings using measured waveform at two photoelectric detectors 10-1 and 10-2, and divides Ji Suan not two phase shifts.Measured waveform produces the first phase shift between joint 4 and polarizer 9-1 at detector 10-1, and measured waveform at the detector 10-2 produces the second phase shift between joint 4 and polarizer 9-2
Therefore, two differences of measurement phase shiftCorresponding to the phase shift inside sensing medium 8.The differential phase is surveyed AmountDo not influenceed by any phase shift variations between polarizer 2 and beam splitter 7, as long as MPD modulating frequencies are far above disturbance frequency Rate so that disturbance passes throughWithMeasure simultaneously and comparably track, and be therefore subtracted completely.
For voltage measurement, electro-optic crystal can act as sensing medium 8, so as to by voltage conversion to be measured into crystal Phase shift between orthogonal polarization mode.There is no electro-optic crystal (such as Bi of natural birefringence4Ge3O12, BGO) be preferred.Electricity Fiber waveguide or optical fiber can also act as voltage sensing medium.The end face (being cut along [001] direction) of BGO crystal is electrically connected to electricity Pole, it provides voltage drop V.
As mentioned, there is two kinds of MPD signal transactings configuration (and referring to bibliography [8]):Open loop and closed loop. In general, closed loop configurations are than open loop homologue(counterpart)Be more difficult to realize, but sensor output stability and Linearity aspect is excellent.
In open-loop configuration, phase-modulator applies self-excitation modulation, and phase shift by signal processing unit 11 from measurement ripple Shape is calculated.A kind of typical case realizes described in patent US 6429939 (bibliography [13]), wherein being adjusted using sinusoidal phase β (t) processed, and phase shift is calculated from the relative ratios of the various harmonic powers in measured waveform.
In Open-loop sensors, the feedback to modulation waveform is not carried out from the phase shift for being calculated, except modulation amplitude Outside license energy (but not being forcibly) is stablized using the output calculated from measured waveform.
By contrast, in closed loop configurations [8], the skew of phase-modulation waveform (or equivalent 2 π amplitude zig-zags Phase) pass through to calculate the opposite continuous adjustment of phase shift via feedback control loop so that the phase shift operating point of sensor remains Fixing point (such as zero).Detector and phase-modulator are linked in the feedback loop via signal processing unit 11, wherein institute The phase shift of retrieval is fed back to control phase-modulation waveform.
In differential MPD schemes of the invention, there are at least two detectors, but there is normally only a phase-modulation Device.Therefore, it is not possible to two kinds of detector output operation closed loop detections.Can realize to two kinds of open loop signals of detector output Treatment;Or it is alternatively possible to realize to detector output one of them (such as detector 10-1) closed signal treatment, And process from another detection signal (such as detector 10-2) to extract phase shift using open loop signal.
If the closed signal treatment to detector 10-1 is realized in selection, will to the phase shift of polarizer 9-1 from tap points 4 Remain at and value (such as zero) is fixedly installed.In this case, the phase shift of sensing medium 8 is in detector 10-2 places The phase shift of measurement subtracts arranges value, and does not need further subtracting between institute's detection signal generally.
The second aspect of the present invention is related to the coherence of the light generated by light source 1.Although MPD phase measurement principles will Worked together with high-coherence light source, such as laser of narrowband diode, but in fact, broad band source, example with short coherence time If superluminescent LED (SLED) is often preferred, so as to location interference ripple, and avoid being coupled from various optical fiber Point(junction)The cross-linked parasitic disturbances at place.Using this low-coherence light source, can only be observed in relatively short scope To interference signal, relative group of delay between two of which polarization was completely within the coherence time of source, and outside it, it is right to disturb Rapid decrease and zero will be finally dropped to than degree, and MPD Phase Detecting Devices will be stopped.
Therefore, if using low-coherence light source, various birefringence components, such as PM optical fiber and modulator in system must Design and balance its intrinsic relative group must be adjusted to postpone so that the total phase between tap points 4 and output polarizer 9-1 and 9-2 Postpone to remain minimum and fall completely within the coherence time of light source to group.For this purpose, additional group of delay is mended It can be preferred to repay during element inserts wave path.
However, with changes in environmental conditions, the temperature and stress sensitive of component and possible non-homogeneous environment in system Degree remains able to make total relative group delay slow drift leave minimal design value.Therefore, environmental perturbation is excessive wherein and/or light In coherence time in source too short sensing system, may certify that it is advantageous that active stabilization always relative group postpones or equivalent Stabilization interference contrast, successfully to realize differential MPD schemes.This is it is naturally required that measurement and the interference of control MPD signals are right Than the ability of degree.
Although MPD schemes are routinely only used for measuring phase shift, it is possible that extension signal processing algorithm, and also from survey Signal is measured to draw interference contrast.Many to realize existing, this depends on the factor of such as modulation waveform and feedback control configuration. Below, the example procedure for being calculated come description disturbance contrast using the Sine Modulated waveform of open-loop configuration, it is patent US The extension of the algorithm described in 6429939 (bibliography [13]).
Phase-modulator 5 is connected with sensing medium 8, is added to phase shift to be measured so as to additional phase shift is modulated into β (t)。 Modulation luminous power after detector, detector 10-2 measurements linear polarization, such as polarizer 9-2 of such as Fig. 1.Modulation inspection Surveying device signal can write
[1]
Wherein I0The power output of light source is represented,Be in the phase shift to be measured of the central wavelength of ripple, and A be interference Contrast.
Using Sine Modulated, the detector signal of equation [1] can write according to fourier expansion It is a series of harmonic of the different rank k in modulating frequency Ω, i.e.
[1']
Wherein first three harmonic amplitude BkAnd phaseFor
Use the first species JkThe Bessel function of (β).The symbol of harmonic component can by by the phase of harmonic component with swash The phase for encouraging waveform is compared to determine.
Vector or plural number can be formed from above-mentioned expression, and it allows to draw phase shift main value from institute's detection signalWith it is dry Disturb contrast A.
[2]
Phase shift main valueThe independent variable of Y can be calculated as, and interference contrast A is equal to its absolute value divided by I0.Total optical power I0Can be calculated as
It is preferred that modulation amplitude is β=1.84 rad, wherein J1(β) has its first maximum number;Another preferred amplitude is β=2.63 rad, wherein J1(β) and J2(β) is equal.But, generally, for the MPD methods for work, phase-modulation width Degree β can be arbitrarily small.Additionally, for example for the purpose of stable amplitude, it is known that modulation amplitude β also can be from measurement harmonic wave Amplitude is calculated.The other details of open loop MPD signal transactings can see bibliography [8,13].
In the example of fig. 1, the additional measurement of interference contrast or any parameter associated therewith or equivalent is expressed as IC。
Simultaneously as the interference contrast of MPD signals can be by environmental perturbation, so it also can be by controlling environment bar Part is controlled.As indicated by the arrow IC in Fig. 1, institute's determination value of interference contrast or any coherent signal can be used for controlling At least some parameters of sensor processed.
A kind of possibility is the temperature of the phase-modulator in heater to be controlled or peltier unit.As temperature becomes Change, the birefringence of modulator crystal and relative group postpone also to change.Similarly, it is also possible to control the temperature of the section of PM optical fiber Or strain.Realize that the other method of this interference contrast control also can be easily designed.
Using measurement and controlling mechanism, then feedback control loop can be set up, to stablize MPD interference contrasts, to prevent it It is drifted away from coherent ranges.But, feedback had both been needed not be accurately also without being quick, because the coherent ranges of light source It is usually moderate, and possible group of delay drift is actually also slow.
Next, proposing several examples of relative group delay compensation in the design of sensor.
In the example of Fig. 2A, two substantially the same birefringent phase modulators 5 and 5' are spelled with 90 ° of relative axle alignment It is connected together, therefore its intrinsic birefringence is cancelled.The length of the PM optical fiber 3 between 45 ° of tap points and 90 ° of tap points 4' should be with PM fiber lengths between 90 ° of tap points 4' and collimator 6 are identical so that its birefringence is also cancelled.Phase-modulator 5' and PM optical fiber between tap points 4' and collimator 6 collectively forms group delay compensation component 20.At least some energy of birefringence component Enough it is maintained in housing 21, to keep the uniform environment among them and shield(shield against)Stress and temperature wave It is dynamic.The PM fiber segments 3 stayed in outside housing 21 are preferably held as short as possible.Meanwhile, MPD phase-modulations can be distributed in two Between individual phase-modulator 5 and 5', so as to allow each modulator may to be operated in more small range with the more preferable linearity.
The example of Fig. 2 B is similar with Fig. 2A, and wherein difference is, using only a phase-modulator 5, and phase-modulation The intrinsic birefringence of device crystal 5 is (signified by ring in Fig. 2 B by serving as one of section of PM optical fiber 3 of group delay compensation component 20 Show) in extra length compensate.Housing 21 can similarly include at least some of birefringence component.Because phase-modulator The temperature characterisitic of crystal 5 and PM optical fiber 3 can be different, so with the temperature change of sensor, this design can be subjected to Postpone drift than designing many groups shown in Fig. 2A.
If low-coherence light source is used as source 1, the measurement of IC is with the another of ambiguousness removal and measurement range extension relatively Outer benefit, if being described as follows:
The phase-shift measurement of sensor is disturbed typically inherently in terms of 2 π cycles(periodwise)It is ambiguity.But, low phase The auto-correlation function (being defined as disturbing contrast herein) in dry source is narrow function, and its value is within its coherence time from a phase Bit period is to another phase cycling significant changes.Therefore, if simultaneously measurement phase shift main value ((- π ,+π] within phase shift it is exhausted To value(mod)2 π) and interference contrast, then auto-correlation function has the model of the strongly monotone correlation postponed to relative group wherein In enclosing, interference contrast can be used for phase shift main value measured by correct period allocated, and thus clearly determine relative phase The value completely moved.
Thus, for example according to equation [2] to relative phase shift and IC (or any relevant parameter) while measurement can be Outside being used for for phase-shift measurement scope expanding to 2 π in sensor of the invention, effectively extend to by the auto-correlation letter of light source The slope and scope determined by form of number (or cross-correlation function, if ripple passes through two not homologous generations).
Such as can be also employed in conjunction with using any other cycle clear one's mind of doubt method of two different wave lengths, so as to Outside clear and definite phase-shift measurement scope expanded into 2 π.In patent application WO 9805975A1 [6] and EP 1179735A1 [7] The example of this kind of method is described.The third aspect of the present invention is related to the geometry designs of sensor.Fig. 1 shows transmission configuration sensor Example, wherein light source 1 (and many other components) and detector 10-2 be located at sensing crystal two opposite ends.For voltage The example of sensor, this causes some components, particularly one of detector 10-1 or 10-2 to be located at high-voltage.Fig. 3 Illustrate the example of reflection configuration voltage sensor.In reflection configuration, reflective optical device 30 is placed on one end of sensing element 8 (one end preferably at high-voltage), and every other optics is located at the other end (preferably at ground potential End).Reflective optical device 30 can be flat/curved reflectors, roof type speculum, corner cube retrodirective reflector or only It is deposited on the reflective film coating on crystal end-face.Reflection at reflective optical device 30 should ideally preserve the polarization shape of light State, without rotating or polarizing dependent phase shift.Element 20 represent again described in during as discussed above concerning Fig. 2A and Fig. 2 B (one or It is multiple) optional group of delay compensation component.
The electric light axle of crystal should abreast align with the axle of PM optical fiber 3.Preferably, the beam splitter 7 before sensing medium 8 Should be alignd with its axle with 45 ° relative to PM fiber axis, so as to any possible phase for making two interference ripples to be experienced from beam splitter Phase shift etc..Any remaining system of the remaining natural birefringence for example from beam splitter, retrodirective reflector or from BGO crystal Phase shift can be characterized and removed by calibrating.The residual birefringence of BGO can also be dropped by two BGO crystal of tandem compound Low, wherein antiparallel [001] axle and x/y axles are rotated relatively to each other 90 °.In this arrangement, electric light phase shift is added up to, and this Birefringence cancellation is levied, so as to cause more preferable zero stability.Detector 10-1 or 10-2 can be directly attached to its of sensor Remaining part point, or alternatively, they can be connected to sensor via single mode or multimode fibre.
Although some currently preferred embodiments of the present invention is illustrated and described herein, it is to be appreciated that the invention is not limited in This, but can implement and embody by different way in addition within the scope of claims below.
Cited bibliography
List of reference characters
Light source 1
Linear polarizer 2
Polarization keeps (PM) optical fiber 3
Fibre-optical splice 4,4'
Optical phase modulator 5,5'
Collimator 6
Beam splitter 7
Sensing element 8
Linear polarization 9-1,9-2
Fluorescence detector 10-1,10-2
Signal processing unit 11
Group postpones biasing element 20
Control housing 21
Reflective optical device 30.

Claims (15)

1. one kind interferes determination sensor, including
Sensing element (8), thus measurand add two ripples between relative phase shift,
At least the first and second detectors (10-1,10-2),
Separator element (7), wherein the first output branch of the separator element goes to first detector (10-1), and And the second output branch of the separator element is by the sensing element (8) and goes to second detector (10-2) On,
Characterized in that, the sensor also includes phase-modulator (5), it causes the modulation to the relative phase shift,
Wherein described separator element is located between the phase-modulator (5) and the sensing element (8),
Wherein described first detector (10-1) is not included described in as caused by the measurand in response to relative phase shift Relative phase shift and detect interference signal, and wherein described second detector (10-2) in response to relative phase shift include by the quilt Survey the relative phase shift caused by object and detect interference signal,
The sensor also includes signal processing unit (11), and it is adapted to determine described two from detected interference signal each Relative phase shift between individual ripple, and determine measurand value using the amount for representing their difference.
2. sensor as claimed in claim 1, also postpones biasing element (20), to control in first detector including group Described relative group between the ripple of (10-1) place and the detection of second detector (10-2) place postpones.
3. sensor as claimed in claim 2, wherein, described group of delay biasing element (20) including with birefringence axis (4') 90 ° of change the polarization-maintaining fiber (3) for being connected to other sections at least one sections.
4. sensor as claimed in claim 2, wherein, described group of delay biasing element (20) including with the phase-modulator (5) substantially the same at least second phase modulator (5'), wherein described two modulators with the birefringence axis (4') 90 ° of transformations are connected to each other.
5. the sensor as any one of claim 2 to 4, wherein, described group of delay biasing element (20) and the phase Position modulator (5) is in common housing (21) or temperature controlled.
6. such as sensor in any one of the preceding claims wherein, wherein, the separator element (7) is bulk optical beam splitting Device or multiple-limb fiber coupler.
7. such as sensor in any one of the preceding claims wherein, wherein, the signal processing unit (11) is adapted to from described Any value and the relative phase shift that interference contrast (IC) is represented to draw of interference signal.
8. such as sensor in any one of the preceding claims wherein, wherein, the phase-modulator (5) is electric light phase-modulation Device, integrated optic phase modulator, specifically birefringence modulator, Y type modulators or piezoelectric fibers modulator.
9. such as sensor in any one of the preceding claims wherein, wherein, the phase-modulator is in closed feedback loop One of interference signal is detected using two to control, and wherein described measurand is from another detected interference signal To draw, changed by the arranges value of the closed feedback loop.
10. such as sensor in any one of the preceding claims wherein, wherein, the ripple is light wave, specifically cross line Property polarized lightwave or left and right circular polarization light wave.
11. such as sensor in any one of the preceding claims wherein, wherein, the measurand is voltage or electric-field intensity, And the relative phase shift inside the sensing element is in response to the voltage that is applied between its two faces.
12. such as sensor in any one of the preceding claims wherein, wherein, the sensing element includes electro-optic crystal or electric light Fibre, specifically crystallizes electric light fibre or polarization electric light fibre or optical fiber and piezoelectric.
13. sensor as described in claim 11 or 12, as reflection configuration sensor, wherein reflective optical device (30) edge Same paths return to the ripple by the sensing element.
14. such as sensor in any one of the preceding claims wherein, wherein, the sensing element includes magneto-optic memory technique or light It is fine.
15. such as sensor in any one of the preceding claims wherein,
Wherein, the modulation as caused by the phase-modulator (5) is unrelated with the measurand, and
Wherein described signal processing unit (11) is adapted to from the modulation as caused by the phase-modulator (5) to determine State the relative phase shift between two ripples.
CN201580009312.1A 2014-02-21 2015-02-19 Interference determination sensor with differential modulated phase-detection Active CN106796125B (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
EP14156092.0 2014-02-21
EP14156092 2014-02-21
PCT/EP2015/053516 WO2015124678A1 (en) 2014-02-21 2015-02-19 Interferometric sensor with differential modulated phase detection

Publications (2)

Publication Number Publication Date
CN106796125A true CN106796125A (en) 2017-05-31
CN106796125B CN106796125B (en) 2019-06-18

Family

ID=50137559

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201580009312.1A Active CN106796125B (en) 2014-02-21 2015-02-19 Interference determination sensor with differential modulated phase-detection

Country Status (3)

Country Link
CN (1) CN106796125B (en)
DE (1) DE112015000886T5 (en)
WO (1) WO2015124678A1 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP3290870B1 (en) 2016-09-02 2019-03-13 ABB Schweiz AG Closed-loop interferometric sensor using loop gain for determining interference contrast
EP3290931B1 (en) * 2016-09-02 2019-05-15 ABB Schweiz AG Interferometric voltage sensor with error compensation
CN114325030B (en) * 2021-09-30 2024-05-03 南京曦光信息科技研究院有限公司 Double-square-wave modulation open-loop demodulation method based on optical current transformer

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3707329A (en) * 1970-02-25 1972-12-26 Bbc Brown Boveri & Cie Apparatus for electronically analyzing modulated light beams
US5308973A (en) * 1990-11-22 1994-05-03 Hilti Aktiengesellschaft Method and device for the measurement of force by a fiber optics system by evaluating phase shift of light waves
DE19544778A1 (en) * 1995-11-30 1997-06-05 Siemens Ag Method and arrangement for measuring a measured variable, in particular an electrical current, with high measurement resolution
CN101155162A (en) * 2006-09-28 2008-04-02 冲电气工业株式会社 Otdm-dpsk signal generator capable of detecting an optical carrier phase difference between optical pulses
CN101334427A (en) * 2008-07-16 2008-12-31 上海大学 Reflecting type full-optical fiber current sensor
CN101568842A (en) * 2006-12-22 2009-10-28 Abb研究有限公司 Optical high voltage sensor
CN101600968A (en) * 2006-12-22 2009-12-09 Abb研究有限公司 Optical voltage sensor
CN102109414A (en) * 2010-12-15 2011-06-29 深圳大学 Method and device for calibrating phase modulation of spatial light modulators by utilizing heterodyne interference

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5402234A (en) * 1992-08-31 1995-03-28 Zygo Corporation Method and apparatus for the rapid acquisition of data in coherence scanning interferometry

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3707329A (en) * 1970-02-25 1972-12-26 Bbc Brown Boveri & Cie Apparatus for electronically analyzing modulated light beams
US5308973A (en) * 1990-11-22 1994-05-03 Hilti Aktiengesellschaft Method and device for the measurement of force by a fiber optics system by evaluating phase shift of light waves
DE19544778A1 (en) * 1995-11-30 1997-06-05 Siemens Ag Method and arrangement for measuring a measured variable, in particular an electrical current, with high measurement resolution
CN101155162A (en) * 2006-09-28 2008-04-02 冲电气工业株式会社 Otdm-dpsk signal generator capable of detecting an optical carrier phase difference between optical pulses
CN101568842A (en) * 2006-12-22 2009-10-28 Abb研究有限公司 Optical high voltage sensor
CN101600968A (en) * 2006-12-22 2009-12-09 Abb研究有限公司 Optical voltage sensor
CN101334427A (en) * 2008-07-16 2008-12-31 上海大学 Reflecting type full-optical fiber current sensor
CN102109414A (en) * 2010-12-15 2011-06-29 深圳大学 Method and device for calibrating phase modulation of spatial light modulators by utilizing heterodyne interference

Also Published As

Publication number Publication date
CN106796125B (en) 2019-06-18
WO2015124678A1 (en) 2015-08-27
DE112015000886T5 (en) 2016-11-10

Similar Documents

Publication Publication Date Title
EP1476721B1 (en) (fiber) optic sensor with proper modulation
US6122415A (en) In-line electro-optic voltage sensor
AU777637B2 (en) Fiber-optic current sensor
CN105051551B (en) Fibre optic current sensor with spun optical fiber and temperature-compensating
JP2866186B2 (en) Electromagnetic field strength measuring device
EP3011270B1 (en) Dynamically monitoring the instantaneous zero rotation rate voltage of interferometric fiber optic gyroscope (ifog)
CN105992934B (en) Interferometric sensor
CN108036783A (en) Non-interfering formula optical gyroscope and sensing spinning solution based on polarization detection technology
US20030103211A1 (en) Sensor and method for detecting fiber optic faults
CN102692314A (en) Apparatus and method for testing power spectral density of frequency noise of laser based on fiber resonator
CN101886925A (en) Multi-wavelength interference type optical fiber gyro based on carrier modulation
CN106062506B (en) Interferometric sensor
KR101923705B1 (en) a optic-fiber current sensor system
CN106796125B (en) Interference determination sensor with differential modulated phase-detection
CN109477860B (en) Sensor device with integrated beam splitter
KR101841722B1 (en) apparatus for measuring current and temperature using light
Yu et al. Influence of polarization-dependent crosstalk on scale factor in the in-line Sagnac interferometer current sensor
CN107806981B (en) Measuring device for beat length of polarization maintaining optical fiber
Li et al. IFOG Based on Rhombic Optical Path Difference Bias Configuration for High-Frequency Angular Vibration Measurement
WO2012163923A1 (en) Fiber-optic voltage sensor
GB2256044A (en) Fibre-optic sensor
Kublanova et al. Study of an interferometric fiber-optic gyroscope with a birefringence modulator
CN107101805B (en) Hollow polarization-maintaining photonic crystal fiber Verdet constant measuring apparatus and method
RU2234680C2 (en) Method for stabilizing scaling factor of optic fiber gyroscope
Nascimento Optical fiber sensors technology for supervision, control and protection of high power systems

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant
TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20210702

Address after: Baden, Switzerland

Patentee after: ABB grid Switzerland AG

Address before: Baden, Switzerland

Patentee before: ABB Switzerland Co.,Ltd.

CP03 Change of name, title or address
CP03 Change of name, title or address

Address after: Swiss Baden

Patentee after: Hitachi energy Switzerland AG

Country or region after: Switzerland

Address before: Swiss Baden

Patentee before: ABB grid Switzerland AG

Country or region before: Switzerland

TR01 Transfer of patent right
TR01 Transfer of patent right

Effective date of registration: 20240218

Address after: Zurich, SUI

Patentee after: Hitachi Energy Co.,Ltd.

Country or region after: Switzerland

Address before: Swiss Baden

Patentee before: Hitachi energy Switzerland AG

Country or region before: Switzerland