[go: up one dir, main page]

CN118896636B - A method, system and device for demodulating and anti-aliasing measurement of optical fiber F-P sensor - Google Patents

A method, system and device for demodulating and anti-aliasing measurement of optical fiber F-P sensor Download PDF

Info

Publication number
CN118896636B
CN118896636B CN202411381020.8A CN202411381020A CN118896636B CN 118896636 B CN118896636 B CN 118896636B CN 202411381020 A CN202411381020 A CN 202411381020A CN 118896636 B CN118896636 B CN 118896636B
Authority
CN
China
Prior art keywords
sampling rate
module
sampling
signal
rate
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.)
Active
Application number
CN202411381020.8A
Other languages
Chinese (zh)
Other versions
CN118896636A (en
Inventor
马志波
李若飞
喜奇
苑曦宸
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.)
Northwestern Polytechnical University
Original Assignee
Northwestern Polytechnical University
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 Northwestern Polytechnical University filed Critical Northwestern Polytechnical University
Priority to CN202411381020.8A priority Critical patent/CN118896636B/en
Publication of CN118896636A publication Critical patent/CN118896636A/en
Application granted granted Critical
Publication of CN118896636B publication Critical patent/CN118896636B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F17/00Digital computing or data processing equipment or methods, specially adapted for specific functions
    • G06F17/10Complex mathematical operations
    • G06F17/11Complex mathematical operations for solving equations, e.g. nonlinear equations, general mathematical optimization problems
    • G06F17/12Simultaneous equations, e.g. systems of linear equations
    • 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
    • G01D5/35312Mechanical 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 Fabry Perot
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H9/00Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means
    • G01H9/004Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means using fibre optic sensors
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L1/00Measuring force or stress, in general
    • G01L1/24Measuring force or stress, in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infrared, visible light, ultraviolet
    • G01L1/242Measuring force or stress, in general by measuring variations of optical properties of material when it is stressed, e.g. by photoelastic stress analysis using infrared, visible light, ultraviolet the material being an optical fibre
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L11/00Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00
    • G01L11/02Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00 by optical means
    • G01L11/025Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00 by optical means using a pressure-sensitive optical fibre

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Mathematical Physics (AREA)
  • Computational Mathematics (AREA)
  • Mathematical Analysis (AREA)
  • Mathematical Optimization (AREA)
  • Pure & Applied Mathematics (AREA)
  • Data Mining & Analysis (AREA)
  • Theoretical Computer Science (AREA)
  • Operations Research (AREA)
  • Databases & Information Systems (AREA)
  • Software Systems (AREA)
  • General Engineering & Computer Science (AREA)
  • Algebra (AREA)
  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)
  • Optical Communication System (AREA)

Abstract

The invention discloses a demodulation anti-aliasing measurement method, a demodulation anti-aliasing measurement system and demodulation anti-aliasing measurement equipment for an optical fiber F-P sensor, and belongs to the technical field of demodulation of optical fiber sensors. Aiming at the problem of frequency aliasing caused by incapability of measuring high-frequency signals due to insufficient bandwidth of the existing fiber F-P sensor demodulation system, the invention adopts the self-adaptive sampling technology and the self-adaptive model reference control, and adjusts the sampling rate of the system in real time according to the frequency information of the acquired signals so as to realize higher precision and resolution in a key area, dynamically adjust the allocation of computing resources, improve the accuracy of integral sampling rate and signal reconstruction, enhance the robustness of the system and effectively cope with challenging vibration environment conditions. Compared with the traditional method, the method not only solves the problem of bandwidth limitation, but also improves measurement accuracy, stability and robustness, and provides a high-efficiency and reliable solution for F-P sensor vibration and pressure measurement in extreme environments.

Description

Demodulation anti-aliasing measurement method, system and equipment for optical fiber F-P sensor
Technical Field
The invention relates to the technical field of demodulation of optical fiber sensors, in particular to a demodulation anti-aliasing measurement method, a demodulation anti-aliasing measurement system and demodulation anti-aliasing measurement equipment for an optical fiber F-P sensor.
Background
Fiber optic F-P sensors are one type of sensor commonly used for vibration measurement and pressure monitoring in extreme environments, however, random vibration links present challenges to the performance of the F-P sensor because the optical path length within the F-P air cavity is affected by vibration under varying vibration environmental conditions to produce linear changes. According to the Nyquist sampling law, at this time, if the spectrum sampling rate is lower than the highest frequency twice of the vibration signal, the measured F-P cavity length value will be caused to generate a periodical aliasing phenomenon, so that the accuracy and stability of the cavity length data under the measurement of the high-frequency signal are reduced. Such aliasing errors can affect the reliability of experimental results, leading to severe distortion of signal waveforms and instability of frequency measurements. Thus, there is an urgent need for a new solution that can effectively address this challenge. To solve this problem, it is common to use increasing the sampling rate of a spectrometer as an anti-aliasing means, or to splice spectral signals using a multi-channel spectrometer, and by increasing the sampling rate, the bandwidth of the measurement system can be increased, and the upper limit of the measurable signal frequency can be increased.
The invention patent application document with the application number 202011413621.4 discloses a self-adaptive infrared sensor signal sampling algorithm, the validity and stability of sampling data are improved by taking mean square error as a judging condition, the reliability and the robustness of a temperature measurement result are ensured, and the calculation resources are optimized to a certain extent by dynamically adjusting the quantity of the sampling data. The invention patent application document with the application number 202110509184.4 discloses a high-frequency anti-aliasing band-pass optical analog-digital conversion device, which realizes the anti-aliasing of digital signals through band-pass filtering and non-aliasing digitization of the signals. However, neither of these methods takes into account the allocation and instantaneity of the computing resources, so that demodulation accuracy and resolution cannot be guaranteed.
In addition, the frame rate of the spectrometer limits the demodulation bandwidth of the sensor demodulation system, thereby limiting the application of the demodulation system in high-frequency dynamic pressure measurement. Therefore, the method has great significance in improving the frame frequency of spectrum acquisition and further improving the demodulation bandwidth of the optical fiber F-P sensor. A time-sharing exposure and spectrum signal fusion technology is adopted, a plurality of spectrometer modules are stacked to form a high-speed spectrometer module, so that the frame frequency of the spectrometer is multiplied, and the high-frame frequency spectrum acquisition is realized. However, this method increases the volume of the demodulation system, making it inconvenient to carry, and non-equidistant sampling caused by cross sampling may also cause errors in the demodulated data.
Disclosure of Invention
Aiming at the problems, the invention aims to provide a demodulation anti-aliasing measurement method, a demodulation anti-aliasing measurement system and demodulation anti-aliasing measurement equipment for an optical fiber F-P sensor, which are used for adjusting the sampling rate in real time based on an adaptive sampling technology and adaptive model reference control, improving the accuracy of the overall sampling rate and signal reconstruction and realizing the demodulation anti-aliasing measurement of the optical fiber F-P sensor.
In order to achieve the above purpose, the technical scheme adopted by the invention is as follows:
the demodulation anti-aliasing measurement method for the optical fiber F-P sensor comprises the following steps:
S1, establishing a sampling rate error model according to a cavity length signal input by a superior demodulation system;
S2, based on a sampling rate error model, determining an adaptive control rate of the sampling rate, so that the sampling rate can be adaptively adjusted when signals are aliased;
s3, further realizing equidistant sampling by a trigonometric fitting function interpolation method on the basis of the sampling rate obtained in the step S2;
And S4, sampling according to the sampling points determined in the step S3, and calculating the signal frequency of the sampling points.
Further, the specific operation of step S1 includes the following steps:
s101, according to the cavity length signal input by the upper demodulation system Determining a sampled signal model;
Wherein n is the number of sampling points,The cavity length signal input for the superior demodulation system, t represents the sampling time,The sampling rate, in Hz,Representing a unit impulse function;
s102, calculating the signal phase at the current sampling rate according to a transfer equation;
s103, calculating the phase in the last sampling rate state according to a reference model;
s104, determining an error function according to the phase difference corresponding to the two adjacent sampling rates;
s105, determining a calculation method of the error e.
Further, in step S102, the signal phase at the current sampling rate is expressed as;
In the formula,The output of the signal is represented by,Which represents the phase of the signal and,Is the first derivative of the phase, i.e. the frequency of the signal, freq is a calculated function of the frequency,Representing the feedback sample signal and,As a control coefficient of the forward channel,Is controlled by
Further, in step S103, the phase in the last sampling rate state is expressed as:;
In the formula, For the signal output in the last sample rate state,Representing the phase of the signal at the last sample rate state,Representing the frequency at the last sample rate state, i.e. the reference model.
Further, the error function in step S104 is expressed as;
Where e denotes the error and f denotes the signal frequency at the current sampling rate, i.eIntroducing parametersAndFor a pair ofControl is performed so as to change the sampling rate,Indicating the direction of adjustment of the sampling rate, positive up-regulation, negative down-regulation,Indicating the adjustment amountIf e is smaller than the error threshold, the sampling rate is larger than twice or more of the highest frequency of the acquired signal, the sampling rate does not need to be improved, and if e is larger than the error threshold, aliasing is indicated.
Further, in step S105, a calculation error e of a fracture function is introduced, where the fracture function is expressed as;
In the formula,The broken part is indicated as a broken part,Extreme points of (2) areIs a zero point of (c).
Further, the specific operation of step S2 includes the following steps:
S201, adjusting the sampling frequency and the initial phase ;
Wherein the method comprises the steps ofThe virtual interpolation point is the real interpolation pointIs an integer;
s202, determining an adaptive control rate;
The adaptive control rate is expressed as ;
S203, determining by gradient descent method:;
Wherein, For the number of iterations,In order for the rate of learning to be high,As a function of the break down,For gradient calculations.
Further, the specific operation of step S3 includes the following steps:
S301, obtaining three points by sampling the three points AndInterpolation to obtain:;
S302, determiningIs a position of (2);
Further, the invention also comprises an optical fiber F-P sensor demodulation anti-aliasing measurement system, wherein the anti-aliasing measurement system comprises a reference model module, a transfer equation module, an error identification module, an adaptive rate adjustment module, an interpolation module and a total control module;
The system comprises a reference model module, an adaptive rate adjusting module, an interpolation module, a total control module, an error identifying module, an adaptive rate adjusting module, a reference model module and a transmission equation module, wherein the reference model module is used for calculating the phase of the last sampling rate state, the transmission equation module is used for calculating the signal phase of the current sampling rate;
The reference model module, the transfer equation module, the error identification module, the adaptive rate adjustment module, the interpolation module and the overall control module are realized based on the anti-aliasing measurement method as described above.
Further, the invention also includes an electronic device comprising at least one processor and a memory communicatively coupled to the processor, wherein the memory stores instructions executable by the processor to enable the processor to perform the optical fiber F-P sensor demodulation anti-aliasing measurement method as described above.
The beneficial effects of the invention are as follows:
1. According to the invention, the self-adaptive sampling technology and the self-adaptive model reference control are adopted, and the sampling rate of the system is adjusted in real time through the interpolation point of the self-adaptive rate according to the frequency information of the acquired signal, so that higher precision and resolution are realized in a key area, the problem of bandwidth limitation is solved, and the allocation of computing resources can be dynamically adjusted, so that the system is ensured to reasonably respond to the continuously-changing requirements and environments.
2. According to the invention, through the interpolation point with the self-adaptive rate, the system can automatically adjust the sampling density according to the signal characteristics so as to ensure that higher precision and resolution are realized in a key area, thereby improving the overall sampling rate and the accuracy of signal reconstruction.
3. The control system based on the adaptive model in the invention iteratively adjusts the controller parameters using an adaptive algorithm. The method not only can provide stability and rapid convergence rate, but also can enhance the robustness of the system to unknown disturbance, effectively cope with challenging vibration environment conditions, provides a high-efficiency and reliable solution for vibration measurement and pressure monitoring in extreme environments, and has wide application prospects in practical engineering.
Drawings
FIG. 1 is a schematic diagram of the measurement of an optical fiber F-P vibration sensor according to the present invention.
FIG. 2 is a schematic diagram illustrating the generation of aliasing in the present invention.
FIG. 3 is a schematic block diagram of demodulation anti-aliasing measurement of an optical fiber F-P sensor according to the present invention.
FIG. 4 is a schematic diagram of multi-channel adaptive sampling anti-aliasing in the present invention.
Detailed Description
In order to enable those skilled in the art to better understand the technical solution of the present invention, the technical solution of the present invention is further described below with reference to the accompanying drawings and examples.
Example 1
An embodiment one provides a demodulation anti-aliasing measurement method for an optical fiber F-P sensor, light in a broadband light source is transmitted through an optical fiber channel, when the light interferes with a vibration sensitive F-P structure in the optical fiber, the light is transmitted back through the optical fiber channel and is transmitted to a demodulation system through a ring structure in the light source, and a regularly-changed sine cavity length data curve can be obtained through demodulation, as shown in fig. 1. Sampling the sine curve obtained after demodulation, if the sampling rate is insufficient, aliasing will occur on the spectrum sidebands, and the frequency of the curve cannot be obtained correctly, as shown in fig. 2. According to the invention, the distance between each frequency band is widened by adaptively increasing the sampling rate, and finally the frequency of the signal is calculated by a frequency demodulation algorithm. The self-adaptive sampling rate increasing is carried out by taking the phase as a judgment basis, if the phase difference between the phase in the previous sampling rate state and the phase in the current state does not exceed a threshold value, the sampling rate does not need to be increased, and if the phase difference between the phase in the previous sampling rate state and the phase in the current state exceeds the threshold value, the sampling rate is proved to be insufficient, and the sampling rate is not required to be increased, as shown in figure 3. According to the method, the sampling rate does not need to be regulated and controlled artificially, and the adaptability of the system to variable frequency signals is improved.
Based on the principle, the anti-aliasing measurement method specifically comprises the following steps:
S1, establishing a sampling rate error model according to a cavity length signal input by a superior demodulation system;
more specifically, S101, according to the cavity length signal input by the superior demodulation system Determining a sampled signal model;
In the invention, the sampling function adopts a Dirac comb function, and a signal model obtained by sampling according to the Dirac comb function is expressed as ;
Wherein n is the number of sampling points,The cavity length signal input for the superior demodulation system, t represents the sampling time,The sampling rate, in Hz,Representing a unit impulse function.
It can be seen from the dirac comb function and the variable fourier series derivation that the frequency domain of the input signal is also a discrete function, so that the frequency spectrum of the input signal is shifted to obtain;
In the formula,Is a constant, T s is the sampling time interval, is the sampling rateIs given in s.
S102, calculating the signal phase at the current sampling rate according to a transfer equation;
At the current sampling rate, the signal phase is calculated by the following formula ;
In the formula,The output of the signal is represented by,Which represents the phase of the signal and,Is the first derivative of the phase, i.e. the frequency of the signal, freq is a calculated function of the frequency,Representing the feedback sample signal and,As a control coefficient of the forward channel,Is controlled by
S103, calculating the phase in the last sampling rate state according to a reference model;
the reference model being an uncontrolled version of the transfer function, i.e ;
In the formula,Outputting the signal in the last sampling rate state; representing the phase of the signal at the last sample rate state, Representing the frequency at the last sample rate state, i.e. the reference model.
S104, determining an error function according to the phase difference corresponding to the two adjacent sampling rates;
The error function of the invention adopts the phase difference corresponding to the adjacent two sampling rates, namely ;
Where e denotes the error and f denotes the signal frequency at the current sampling rate, i.eIntroducing parametersAndFor a pair ofControl is performed to change the sampling rate,Indicating the direction of adjustment of the sampling rate, positive up-regulation, negative down-regulation,Representing the adjustment amount, thereby obtaining;
From the above formula, the initial phase of the next sampling rate can be obtained byIs calculated due toFor introduction ofBinary functions for frequency modulation, so that only control variables are requiredAnd (3) obtaining the product.
Setting an error threshold, if e is smaller than the error threshold, proving that the sampling rate is larger than twice or more of the highest frequency of the acquired signal without increasing the sampling rate, and if e is larger than the error threshold, proving that aliasing occurs, and then, performing interpolation to perform control rate design. Such a design may make the system more stable. At this time inputIs at the inputOn the basis of which the frequency and initial phase of the modulation are shifted.
S105, determining a calculation method of an error e;
in the present invention, the error e is calculated by introducing a break function expressed as ;
In the formula,The broken part is indicated as a broken part,Extreme points of (2) areCan be searched by a gradient descent methodExtreme points of (i.e. getCoefficient at minimum error is obtainedAndI.e. the optimal sampling rate.
Further, step S2 is to determine an adaptive control rate of the sampling rate based on the sampling rate error model, so that the sampling rate can be adaptively adjusted when aliasing occurs in the signal.
Specifically, S201, it can be seen from the impairment function in step S1 that the impairment function includes the phase information of the signal and the sampling rate control factorIf it is desired to achieve and maintain equal spacing, two parameters, namely frequency and initial phase, are adjusted, expressed as;
Wherein the method comprises the steps ofThe virtual interpolation point is the real interpolation pointThe formula can be obtained by taking the integer downAnd (3) withCan obtain a relationship ofCorresponding to oneAnd an initial phaseThat is, by changingThe values are phase controlled.
S202, determining an adaptive control rate;
In the invention, the gradient descent is used for control rate design, and the change rate of the sampling rate is expressed as ;
S203, determining by gradient descent method;
Specifically, a differential operator is introduced,;
Can be deduced to;
From the above, it is possible to control the sampling rate to be foundCalculated as;
Wherein, For the number of iterations,In order for the rate of learning to be high,As a function of the break down,For gradient calculations.
Further, step S3, based on the sampling rate obtained in step S2, further realizing equidistant sampling by a trigonometric fitting function interpolation method;
Specifically, the adjusted adaptive control rate in step S2 can be obtained AndTo achieve equally spaced sampling and continue to reduce the mixing probability, a triangular fitting algorithm is used for interpolation in the present invention. The specific formula is as follows:
By sampling the three points, the following three points can be obtained AndObtained by interpolation:;
Is obtained by transforming the trigonometric function;
Then
The numerical value of the interpolation point can be obtained through the step, the numerical value is inserted at the calculated phase position, and the triangular fitting interpolation sampling rate is improved.
Further, in step S4, sampling is performed according to the sampling points determined in step S3, and the signal frequency of the sampling points is calculated.
Through step S2 and step S3, the sampling rate can be adjusted in real time according to the collected signal frequency information, so that it is ensured that the frequency calculation result is not affected by aliasing and errors are generated in the working interval, as shown in fig. 4.
Example two
The second embodiment provides a demodulation anti-aliasing measurement system of an optical fiber F-P sensor, which comprises a reference model module, a transfer equation module, an error identification module, an adaptive rate adjustment module, an interpolation module and a total control module;
The reference model module is used for calculating the phase in the state of the last sampling rate, and the transfer equation module is used for calculating the signal phase in the current sampling rate; the error recognition module judges whether the error exceeds a threshold value after making a difference on the signal phases calculated by the reference model module and the transfer equation module by the self-adaptive rate adjustment module, if the error does not exceed the threshold value, the self-adaptive rate adjustment module adjusts the sampling rate by the interpolation module, and the total control module calculates and outputs the current signal frequency according to the sampling rate output by the self-adaptive rate adjustment module.
It should be noted that the reference model module, the transfer equation module, the error recognition module, the adaptive rate adjustment module, the interpolation module, and the overall control module are implemented according to the method described in the first embodiment.
Example III
An embodiment III provides an electronic device comprising at least one processor and a memory communicatively coupled to the processor, wherein the memory stores instructions executable by the processor to enable the processor to perform the optical fiber F-P sensor demodulation anti-aliasing measurement method described in embodiment one.
The foregoing has shown and described the basic principles, principal features and advantages of the invention. It will be understood by those skilled in the art that the present invention is not limited to the embodiments described above, and that the above embodiments and descriptions are merely illustrative of the principles of the present invention, and various changes and modifications may be made without departing from the spirit and scope of the invention, which is defined in the appended claims. The scope of the invention is defined by the appended claims and equivalents thereof.

Claims (4)

1.一种光纤F-P传感器解调抗混叠测量方法,其特征在于,包括以下步骤:1. A method for demodulating and anti-aliasing measurement of an optical fiber F-P sensor, characterized in that it comprises the following steps: S1:根据上级解调系统输入的腔长信号,建立采样率误差模型;S1: Establish a sampling rate error model based on the cavity length signal input by the upper demodulation system; S2:基于采样率误差模型,确定采样率的自适应控制率,使信号发生混叠时能够对采样率进行自适应调节;S2: Based on the sampling rate error model, determine the adaptive control rate of the sampling rate so that the sampling rate can be adaptively adjusted when signal aliasing occurs; S3:在步骤S2得到的采样率基础上,进一步的通过三角拟合函数插值方法实现等间隔采样;S3: Based on the sampling rate obtained in step S2, further implementing equal-interval sampling through a triangular fitting function interpolation method; S4:根据步骤S3中确定的采样点进行采样,计算采样点的信号频率;S4: Sampling is performed according to the sampling points determined in step S3, and the signal frequency of the sampling points is calculated; 步骤S1的具体操作包括以下步骤:The specific operation of step S1 includes the following steps: S101:根据上级解调系统输入的腔长信号,确定采样后的信号模型S101: According to the cavity length signal input by the upper demodulation system , determine the signal model after sampling ; 式中,n为采样点数,为上级解调系统输入的腔长信号,t表示采样时间,为采样率,单位为Hz,表示单位冲激函数;Where n is the number of sampling points, is the cavity length signal input by the upper demodulation system, t represents the sampling time, is the sampling rate in Hz, represents the unit impulse function; S102:根据传递方程计算在当前采样率下的信号相位;S102: Calculate the signal phase at the current sampling rate according to the transfer equation; S103:根据参考模型对上一采样率状态下的相位进行计算;S103: Calculate the phase in the previous sampling rate state according to the reference model; S104:根据相邻两个采样率对应的相位差,确定误差函数;S104: determining an error function according to a phase difference corresponding to two adjacent sampling rates; S105:确定误差e的计算方法;S105: Determine a calculation method for the error e ; 步骤S102中,在当前采样率下的信号相位表示为In step S102, the signal phase at the current sampling rate is expressed as ; 式中,表示信号的输出,表示信号的相位,为相位的一阶导,也即信号的频率; freq为频率的计算函数,表示反馈采样信号,为前向通道的控制系数,是受控制的In the formula, Represents the output of the signal, represents the phase of the signal, is the first-order derivative of the phase, that is, the frequency of the signal; freq is the calculation function of the frequency, represents the feedback sampling signal, is the control coefficient of the forward channel, is controlled ; 步骤S103中,上一采样率状态下的相位表示为:In step S103, the phase in the previous sampling rate state is expressed as: ; 式中,为上一个采样率状态下的信号输出,表示上一采样率状态下的信号相位,表示上一采样率状态下的频率,上一采样率状态也即参考模型;In the formula, is the signal output in the previous sampling rate state, Indicates the signal phase in the previous sampling rate state, Indicates the frequency at the previous sampling rate state, which is also the reference model; 步骤S104中误差函数表示为The error function in step S104 is expressed as ; 式中,e表示误差,f表示当前采样率下的信号频率,也即;引入参数进行控制,从而改变采样率,表示采样率的调整方向,上调为正,下调为负,表示调整量,则In the formula, e represents the error, f represents the signal frequency at the current sampling rate, that is, ;Introduce parameters and right Control to change the sampling rate, Indicates the adjustment direction of the sampling rate, upward adjustment is positive, downward adjustment is negative, represents the adjustment amount, then ; e小于误差阈值,则采样率大于采集信号最高频率的两倍及以上,无需提高采样率;若e大于误差阈值,说明发生了混叠;If e is less than the error threshold, the sampling rate is greater than or equal to twice the highest frequency of the acquired signal, and there is no need to increase the sampling rate. If e is greater than the error threshold, aliasing has occurred. 步骤S2的具体操作包括以下步骤:The specific operation of step S2 includes the following steps: S201:调整采样频率和初相位,则S201: Adjust the sampling frequency and initial phase, then ; 其中为虚拟插值点,真实插值点为的下取整数;in is a virtual interpolation point, and the real interpolation point is Take the next integer of ; S202:确定自适应控制率;S202: Determine an adaptive control rate; 自适应控制率表示为The adaptive control rate is expressed as ; S203:用梯度下降的方法确定S203: Determine using gradient descent method : ; 其中,为迭代次数,为学习率,为折损函数,为梯度计算;Among them, The number of iterations, is the learning rate, is the loss function, is the gradient calculation; 步骤S3的具体操作包括以下步骤:The specific operation of step S3 includes the following steps: S301:通过对三个点进行采样,得到三个点;插值得到S301: By sampling three points, three points are obtained , and ; Interpolation is obtained : ; S302:确定的位置;S302: Confirm location; . 2.根据权利要求1所述的一种光纤F-P传感器解调抗混叠测量方法,其特征在于,步骤S105中引入折损函数计算误差e,折损函数表示为2. The optical fiber FP sensor demodulation anti-aliasing measurement method according to claim 1, characterized in that a loss function is introduced in step S105 to calculate the error e , and the loss function is expressed as ; 式中,表示折损,的极值点为的零点。In the formula, Indicates loss, The extreme point of is the zero point of . 3.一种光纤F-P传感器解调抗混叠测量系统,其特征在于:包括参考模型模块、传递方程模块、误差识别模块、自适应率调节模块、插值模块和总控制模块;3. A fiber optic F-P sensor demodulation anti-aliasing measurement system, characterized by comprising a reference model module, a transfer equation module, an error identification module, an adaptive rate adjustment module, an interpolation module and a general control module; 所述参考模型模块用于对上一采样率状态下的相位进行计算,传递方程模块用于计算在当前采样率下的信号相位;误差识别模块对自适应率调节模块对参考模型模块和传递方程模块计算得到的信号相位做差后判断误差是否超过阈值;若误差未超过阈值,则自适应率调节模块通过插值模块进行采样率的调节,总控制模块根据自适应率调节模块输出的采样率进行当前信号频率的计算和输出;The reference model module is used to calculate the phase under the previous sampling rate state, and the transfer equation module is used to calculate the signal phase under the current sampling rate; the error identification module determines whether the error exceeds the threshold after subtracting the signal phase calculated by the adaptive rate adjustment module from the reference model module and the transfer equation module; if the error does not exceed the threshold, the adaptive rate adjustment module adjusts the sampling rate through the interpolation module, and the overall control module calculates and outputs the current signal frequency according to the sampling rate output by the adaptive rate adjustment module; 参考模型模块、传递方程模块、误差识别模块、自适应率调节模块、插值模块和总控制模块基于权利要求1或2所述的抗混叠测量方法实现。The reference model module, the transfer equation module, the error identification module, the adaptive rate adjustment module, the interpolation module and the overall control module are implemented based on the anti-aliasing measurement method described in claim 1 or 2. 4.一种电子设备,其特征在于:所述电子设备包括至少一个处理器;以及与所述处理器通信连接的存储器;其中,所述存储器存储有可被所述处理器执行的指令,所述指令被所述处理器执行,以使所述处理器能够执行权利要求1或2所述的光纤F-P传感器解调抗混叠测量方法。4. An electronic device, characterized in that: the electronic device comprises at least one processor; and a memory communicatively connected to the processor; wherein the memory stores instructions executable by the processor, and the instructions are executed by the processor so that the processor can execute the optical fiber F-P sensor demodulation anti-aliasing measurement method described in claim 1 or 2.
CN202411381020.8A 2024-09-30 2024-09-30 A method, system and device for demodulating and anti-aliasing measurement of optical fiber F-P sensor Active CN118896636B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202411381020.8A CN118896636B (en) 2024-09-30 2024-09-30 A method, system and device for demodulating and anti-aliasing measurement of optical fiber F-P sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202411381020.8A CN118896636B (en) 2024-09-30 2024-09-30 A method, system and device for demodulating and anti-aliasing measurement of optical fiber F-P sensor

Publications (2)

Publication Number Publication Date
CN118896636A CN118896636A (en) 2024-11-05
CN118896636B true CN118896636B (en) 2024-11-29

Family

ID=93264932

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202411381020.8A Active CN118896636B (en) 2024-09-30 2024-09-30 A method, system and device for demodulating and anti-aliasing measurement of optical fiber F-P sensor

Country Status (1)

Country Link
CN (1) CN118896636B (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5095263A (en) * 1990-06-11 1992-03-10 Sundstrand Data Control, Inc. Anti-aliasing for frequency output sensors
US5357544A (en) * 1992-07-21 1994-10-18 Texas Instruments, Incorporated Devices, systems, and methods for composite signal decoding

Family Cites Families (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5793801A (en) * 1996-07-09 1998-08-11 Telefonaktiebolaget Lm Ericsson Frequency domain signal reconstruction compensating for phase adjustments to a sampling signal
US6937912B1 (en) * 1999-04-16 2005-08-30 Orban, Inc. Anti-aliased clipping by band-limited modulation with step functions
US6252464B1 (en) * 1999-10-06 2001-06-26 Cubic Defense Systems, Inc. Numerically-controlled nyquist-boundary hopping frequency synthesizer
JP2011053153A (en) * 2009-09-03 2011-03-17 Yokogawa Electric Corp Optical fiber distribution type measuring device
CN112213560A (en) * 2020-09-01 2021-01-12 东南大学 A high-precision power grid broadband signal measurement method based on Z-ADALINE
CN112269054A (en) * 2020-09-16 2021-01-26 国网安徽省电力有限公司六安供电公司 Power Adaptive Algorithm Based on Improved Prony
CN112697181B (en) * 2020-12-02 2022-07-26 广东工业大学 A frequency modulation-based phase-sensitive optical time-domain reflectometry device and method
CN112964931B (en) * 2021-01-26 2022-07-15 浙江工业大学 Non-ideal multi-damping harmonic signal parameter measurement method based on two-channel undersampling
CN113359369B (en) * 2021-05-11 2023-11-14 上海交通大学 High-frequency anti-aliasing bandpass dimmable analog-to-digital conversion device
CN113536714B (en) * 2021-06-30 2023-08-11 佛山科学技术学院 Method for optimally constructing modulator system
CN115616546A (en) * 2022-10-28 2023-01-17 西北工业大学 A method and system for spatial anti-aliasing orientation estimation based on frequency difference
CN117743736B (en) * 2024-02-19 2024-04-30 西北工业大学 Demodulation method, device and system for optical fiber F-P sensor and storage medium
CN118209142A (en) * 2024-05-11 2024-06-18 哈尔滨工程大学 A high-precision demodulation method based on low-fineness FP interferometer

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5095263A (en) * 1990-06-11 1992-03-10 Sundstrand Data Control, Inc. Anti-aliasing for frequency output sensors
US5357544A (en) * 1992-07-21 1994-10-18 Texas Instruments, Incorporated Devices, systems, and methods for composite signal decoding

Also Published As

Publication number Publication date
CN118896636A (en) 2024-11-05

Similar Documents

Publication Publication Date Title
CN109520429B (en) High-speed measurement system and method for few spectral sampling points of white light interferometric fiber optic sensor
CN102610996A (en) Method and device for rapidly calibrating luminous power
CN102353481A (en) Method and device for complementing temperature and pressure of pressure sensor based on two-dimensional orthogonal function
CN107014367B (en) Method for optimizing dynamic performance of fiber-optic gyroscope
WO2011003347A1 (en) Measureing device and measuring method for continuous physical quantity
CN102624456A (en) A system and method for demodulating optical fiber interference sensing signals
CN118896636B (en) A method, system and device for demodulating and anti-aliasing measurement of optical fiber F-P sensor
CN117804646A (en) Pressure sensor and method for realizing pressure sensing
WO2024245464A1 (en) Method and apparatus for improving precision of fundamental wave measurement
TWI631826B (en) Bandwidth adjusting method and related bandwidth adjusting unit and phase recovery module
CN109959825A (en) A fitting and calibration method of nonlinear voltage-controlled attenuator based on Lagrangian interpolation
CN107104674B (en) Noise power estimation device in electric parameter measurement process
CN112532615B (en) Smart grid worm detection method
CN112468281B (en) High-precision symbol synchronization system
CN110187237A (en) Real-time detection and the synchronized acquisition method and its device for adjusting crystal oscillator output frequency
KR20210075361A (en) Calibration method for characteristic curve of ultrasonic gas meter
CN103344414A (en) PZT modulation factor testing device and testing method
JP2017108408A (en) Apparatus for measuring filtering characteristic, pre-equalizer and optical communication equipment
CN117388785A (en) Calibration method and system for voltage acquisition device
CN102832911B (en) A kind of digital signal recovery method and device
CN110135101A (en) An Algorithm for Optimizing Optical Power Accuracy of PD Detection in Optical Cable Monitoring System
CN112836166B (en) First-order differential algorithm of monitoring data of equal-sampling experiment based on response peak analysis
CN115291158A (en) A method and device for automatic calibration of electrical quantity of a settlement and measurement device
CN102055406B (en) Method and device for processing time sequence difference of driver
CN115372696A (en) Grid Voltage Frequency Calculation Method and Device Based on Recursive Fourier Series

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