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CN113253237B - Railway contact net measuring method and system based on radar system - Google Patents

Railway contact net measuring method and system based on radar system Download PDF

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CN113253237B
CN113253237B CN202110787939.7A CN202110787939A CN113253237B CN 113253237 B CN113253237 B CN 113253237B CN 202110787939 A CN202110787939 A CN 202110787939A CN 113253237 B CN113253237 B CN 113253237B
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CN113253237A (en
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王建
毕钡桢
华洋晟
苏琦斌
黄晓涛
周智敏
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National University of Defense Technology
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/02Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
    • G01S7/41Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00 using analysis of echo signal for target characterisation; Target signature; Target cross-section
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B7/00Measuring arrangements characterised by the use of electric or magnetic techniques
    • G01B7/02Measuring arrangements characterised by the use of electric or magnetic techniques for measuring length, width or thickness
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B7/00Measuring arrangements characterised by the use of electric or magnetic techniques
    • G01B7/16Measuring arrangements characterised by the use of electric or magnetic techniques for measuring the deformation in a solid, e.g. by resistance strain gauge
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L5/00Apparatus for, or methods of, measuring force, work, mechanical power, or torque, specially adapted for specific purposes

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Abstract

本申请涉及一种基于雷达系统的铁路接触网测量方法及接触网测量系统,所述方法应用于包括相互通信的主雷达、从雷达以及主控装置的接触网测量系统,通过主控装置控制两个雷达同步工作,采集相同目标在相同时刻不同视角下的雷达回波,并进行脉冲压缩,然后识别接触网在脉冲压缩图像中的波峰位置,接着利用时间差分干涉技术对波峰复数散射数据做干涉处理,分别得到接触网相对于两个雷达的位移量,然后通过求解二元方程得到接触网的导高形变和拉出值形变,最后通过对导高和拉出值的频谱分析估计接触网的力学参数,本方法具有远程非接触、测量精度高、高效实时性强、操作部署便捷等优点。

Figure 202110787939

The present application relates to a railway catenary measurement method and a catenary measurement system based on a radar system. The method is applied to a catenary measurement system including a master radar, a slave radar and a master control device that communicate with each other. The master control device controls the two The two radars work synchronously, collect radar echoes of the same target at the same time and different viewing angles, and perform pulse compression, and then identify the peak position of the catenary in the pulse compressed image, and then use the time differential interference technology to interfer with the peak complex scattering data. After processing, the displacement of the catenary relative to the two radars is obtained respectively, and then the lead-through deformation and the pull-out value deformation of the catenary are obtained by solving the binary equation. This method has the advantages of remote non-contact, high measurement accuracy, high efficiency and real-time performance, and convenient operation and deployment.

Figure 202110787939

Description

基于雷达系统的铁路接触网测量方法及接触网测量系统Railway catenary measurement method and catenary measurement system based on radar system

技术领域technical field

本申请涉及雷达检测技术领域,特别是涉及一种基于雷达系统的铁路接触网测量方法及接触网测量系统。The present application relates to the technical field of radar detection, and in particular, to a railway catenary measurement method and a catenary measurement system based on a radar system.

背景技术Background technique

铁路接触网与机车顶部的受电弓组成的弓网系统是铁路系统中的关键设备之一,接触网是沿钢轨上方呈“之”字形架设的输电线,为机车提供高速行驶所需的能源。接触网质量直接影响到受电弓的受流性能和列车运行安全,由于接触网沿铁路露天布置,工作环境恶劣,运行时牵引(负荷)电流变化大、车体振动剧烈,使接触网的几何参数和电气参数时刻处于复杂的动态变化之中。接触网按照一定的铁路技术标准进行设计和建设,其主要关键技术指标包括:接触线导高、拉出值等几何参数,接触网拉力、动态振幅等力学参数。合适的几何参数与力学参数可以保证弓网接触的位置和压力满足相关技术规范,否则,如果弓网接触压力过小,将增加离线率,产生电火花或拉弧,电火花将造成接触网和受电弓电烧蚀,降低弓网的使用寿命,拉弧将对牵引电机造成严重的伤害,影响机车的牵引安全;如果弓网接触压力太大,会使受电弓滑板和接触线之间产生较大的机械磨损,降低其使用寿命。弓网系统一旦出现故障停电将会造成行车中断,可能造成安全事故,因此如何准确、快速和自动地检测接触网参数是铁路建设和运维部门的重大需求。The pantograph system composed of the railway catenary and the pantograph on the top of the locomotive is one of the key equipment in the railway system. The catenary is a transmission line erected in a "zigzag" shape along the top of the rail to provide the locomotive with the energy required for high-speed running. . The quality of the catenary directly affects the current receiving performance of the pantograph and the safety of train operation. Because the catenary is arranged in the open air along the railway, the working environment is harsh, the traction (load) current changes greatly during operation, and the vehicle body vibrates violently, which makes the geometry of the catenary. Parameters and electrical parameters are in complex dynamic changes all the time. The catenary is designed and constructed in accordance with certain railway technical standards, and its main key technical indicators include: geometric parameters such as contact wire guide height and pull-out value, and mechanical parameters such as catenary tension and dynamic amplitude. Appropriate geometric parameters and mechanical parameters can ensure that the contact position and pressure of the pantograph and catenary meet the relevant technical specifications. Otherwise, if the contact pressure of the pantograph and catenary is too small, the off-line rate will increase, and sparks or arcs will be generated. The electric ablation of the pantograph will reduce the service life of the pantograph, and the arcing will cause serious damage to the traction motor and affect the traction safety of the locomotive; Produces greater mechanical wear and reduces its service life. Once the pantograph and catenary system fails, power outage will cause traffic interruption and may cause safety accidents. Therefore, how to accurately, quickly and automatically detect catenary parameters is a major requirement for railway construction and operation and maintenance departments.

列车运行速度越高对弓网系统的要求也越高,高速铁路特别是下一代高速铁路对接触网测量的要求也越来越高。目前接触网测量可分为接触式和非接触式测量两类技术途径;接触式传感器包括压力传感器、角位移传感器和加速度传感器等,这些方法会加速弓网系统的磨损,降低其使用寿命。非接触式传感器包括红外热成像检测、光学图像检测和激光扫描检测等,由于接触网的截面积小,加上机车的高速运动,这些传感器也存在较大的局限性。其中红外热成像检测仪无法精密测量几何形变,光学图像检测作用距离有限,激光扫描仪对车辆运动造成的指向误差非常敏感,此外这些非接触式测量方法受光照、雨雪尘雾等恶劣气象气候条件的影响,环境适应性差。The higher the running speed of the train, the higher the requirements for the pantograph system, and the higher and higher requirements for the catenary measurement of high-speed railways, especially the next-generation high-speed railways. At present, catenary measurement can be divided into two technical approaches: contact and non-contact measurement; contact sensors include pressure sensors, angular displacement sensors and acceleration sensors, etc. These methods will accelerate the wear of pantograph and catenary system and reduce its service life. Non-contact sensors include infrared thermal imaging detection, optical image detection and laser scanning detection. Due to the small cross-sectional area of the catenary and the high-speed movement of the locomotive, these sensors also have great limitations. Among them, infrared thermal imaging detectors cannot precisely measure geometric deformation, optical image detection has a limited range, and laser scanners are very sensitive to pointing errors caused by vehicle motion. In addition, these non-contact measurement methods are affected by harsh weather conditions such as sunlight, rain, snow, dust and fog. impact, poor environmental adaptability.

发明内容SUMMARY OF THE INVENTION

基于此,有必要针对上述技术问题,提供一种能够适应各种环境且测量精度高的基于雷达系统的铁路接触网测量方法及接触网测量系统。Based on this, it is necessary to provide a railway catenary measurement method and a catenary measurement system based on a radar system that can adapt to various environments and have high measurement accuracy, aiming at the above technical problems.

一种基于雷达系统的铁路接触网测量方法,所述方法应用于接触网测量系统,所述接触网测量系统包括相互通信的主雷达、从雷达以及主控装置,所述主雷达和从雷达分别分布在铁路两侧,且两者之间的连线与铁路中心线垂直;A railway catenary measurement method based on a radar system, the method is applied to a catenary measurement system, the catenary measurement system comprises a master radar, a slave radar and a master control device that communicate with each other, the master radar and the slave radar are respectively Distributed on both sides of the railway, and the connection between the two is perpendicular to the center line of the railway;

所述铁路接触网测量方法包括:The railway catenary measurement method includes:

所述主控装置根据预设的同步方案发送工作指令至所述主雷达和从雷达;The master control device sends work instructions to the master radar and the slave radar according to a preset synchronization scheme;

所述主雷达和从雷达根据所述工作指令向接触网的同一测量点发射测量信号,且将接收到的雷达回波信号发送至所述主控装置;The master radar and the slave radar transmit measurement signals to the same measurement point of the catenary according to the work instruction, and send the received radar echo signals to the master control device;

所述主控装置分别根据主雷达及从雷达发送的初始观测时刻的雷达回波信号进行脉冲压缩得到相应的脉冲压缩图像,且分别识别出接触网在各所述脉冲压缩图像中的波峰位置,以及获取所述波峰位置对应的波峰复数散射数据;The main control device performs pulse compression according to the main radar and the radar echo signal at the initial observation time sent from the radar to obtain corresponding pulse compression images, and respectively identifies the peak positions of the catenary in each of the pulse compression images, and acquiring the wave crest complex scattering data corresponding to the wave crest position;

从预设的局部坐标系中提取所述主雷达和从雷达的实际坐标,根据各所述实际坐标以及相应的波峰复数散射数据进行计算,得到初始观测时刻所述接触网分别与主雷达和从雷达之间的初始距离以及所述接触网的初始坐标;The actual coordinates of the main radar and the slave radar are extracted from the preset local coordinate system, and the calculation is performed according to the actual coordinates and the corresponding wave peak complex scattering data to obtain the contact net at the initial observation time. the initial distance between the radars and the initial coordinates of the catenary;

根据多个观测时刻的雷达回波数据分别得到对应所述主雷达和从雷达的两组复散射观测向量,并根据两组所述复散射观测向量采用时间差分干涉方法得到每一观测时刻所述接触网分别相对于主雷达和从雷达之间的位移量;Two sets of complex scattering observation vectors corresponding to the master radar and the slave radar are obtained according to the radar echo data at multiple observation times, and the time difference interference method is used to obtain the complex scattering observation vectors at each observation time according to the two sets of complex scattering observation vectors. The displacement of the catenary relative to the master radar and the slave radar, respectively;

根据所述主雷达、从雷达的实际坐标、接触网的初始坐标、所述接触网分别与主雷达和从雷达之间的初始距离、以及每一观测时刻所述接触网分别相对于主雷达和从雷达之间的位移量,基于两点间求距离公式构建接触网的导高变化量及拉出值变化量为未知数的方程,并进行求解得到所述导高变化量以及拉出值变化量;According to the actual coordinates of the main radar and the subordinate radar, the initial coordinates of the catenary, the initial distance between the catenary and the main radar and the subordinate radar respectively, and the relative relationship between the catenary and the main radar and the subordinate radar at each observation moment. From the displacement between the radars, based on the formula for finding the distance between two points, construct the equations in which the change of the guide height and the change of the pull-out value of the catenary are unknowns, and solve the equation to obtain the change of the guide height and the change of the pull-out value. ;

根据所述导高变化量以及拉出值变化量进行频谱分析得到所述接触网的力学参数。The mechanical parameters of the catenary are obtained by spectrum analysis according to the variation of the lead height and the variation of the pull-out value.

在其中一实施例中,所述预设的同步方案包括第一同步方案和第二同步方案;In one of the embodiments, the preset synchronization scheme includes a first synchronization scheme and a second synchronization scheme;

所述第一同步方案包括控制所述主雷达和从雷达在相同时刻发射波形为不同频率或不同编码的测量信号;The first synchronization scheme includes controlling the master radar and the slave radar to transmit measurement signals with waveforms of different frequencies or codes at the same time;

所述第二同步方案包括控制所述主雷达和从雷达交替发射波形为相同频率和相同编码的测量信号。The second synchronization scheme includes controlling the master radar and the slave radar to alternately transmit measurement signals of the same frequency and the same encoding.

在其中一实施例中,所述主雷达和从雷达发射的测量信号带宽大于500MHz。In one of the embodiments, the bandwidth of the measurement signals transmitted by the master radar and the slave radar is greater than 500 MHz.

在其中一实施例中,所述主控装置根据预设的同步方案发送工作指令至所述主雷达和从雷达之后包括:In one of the embodiments, after the master control device sends a work instruction to the master radar and the slave radar according to a preset synchronization scheme, it includes:

所述主雷达和从雷达根据所述工作指令向接触网的同一测量点发射测量信号,接收到的雷达回波信号后,分别对所述雷达回波信号进行脉冲压缩得到压缩后的雷达回波信号,并将其发送至所述主控装置;The master radar and the slave radar transmit measurement signals to the same measurement point of the catenary according to the work instruction, and after receiving the radar echo signals, pulse compression is performed on the radar echo signals respectively to obtain compressed radar echoes. signal and send it to the master device;

所述主控装置根据所述主雷达及从雷达发送的初始观测时刻的压缩后的雷达回波信号,并将其转换成脉冲压缩图像,识别出接触网在各所述脉冲压缩图像中的波峰位置、以及获取所述波峰位置对应的波峰复数散射数据。The main control device converts the compressed radar echo signal at the initial observation time sent by the main radar and the slave radar into a pulse-compressed image, and identifies the peaks of the catenary in each of the pulse-compressed images. position, and obtain the wave peak complex scattering data corresponding to the wave peak position.

在其中一实施例中,所述从预设的局部坐标系中提取所述主雷达和从雷达的实际坐标,根据各所述实际坐标以及相应的波峰复数散射数据进行计算,得到初始观测时刻所述接触网分别与主雷达和从雷达之间的初始距离、以及所述接触网的初始坐标,其中在得到所述初始观测时刻所述接触网分别与主雷达和从雷达之间的初始距离之后包括:In one embodiment, the actual coordinates of the master radar and the slave radar are extracted from a preset local coordinate system, and the calculation is performed according to each of the actual coordinates and the corresponding wave peak complex scattering data to obtain the data at the initial observation time. The initial distance between the catenary and the main radar and the secondary radar respectively, and the initial coordinates of the catenary, wherein after obtaining the initial distance between the catenary and the main radar and the secondary radar at the initial observation time include:

根据主雷达实际坐标、主雷达与接触网之间的初始距离构建接触网的初始坐标为未知数的第一方程;According to the actual coordinates of the main radar and the initial distance between the main radar and the catenary, construct the first equation in which the initial coordinates of the catenary are unknowns;

根据从雷达实际坐标、从雷达与接触网之间的初始距离构建接触网的初始坐标为未知数的第二方程;According to the actual coordinates of the radar and the initial distance between the radar and the catenary, a second equation with the initial coordinates of the catenary as an unknown number is constructed;

利用第一方程和第二方程进行求解,得到所述接触网的初始坐标。Solve the first equation and the second equation to obtain the initial coordinates of the catenary.

在其中一实施例中,所述根据所述主雷达、从雷达的实际坐标、接触网的初始坐标、所述接触网分别与主雷达和从雷达之间的初始距离、以及每一观测时刻所述接触网分别相对于主雷达和从雷达之间的位移量,基于两点间求距离公式构建接触网的导高变化量及拉出值变化量为未知数的方程,并进行求解得到所述导高变化量以及拉出值变化量包括:In one embodiment, the method is based on the actual coordinates of the main radar and the subordinate radar, the initial coordinates of the catenary, the initial distances between the catenary and the main radar and the subordinate radar respectively, and the data obtained at each observation moment. The above-mentioned catenary is respectively relative to the displacement between the main radar and the slave radar. Based on the formula for calculating the distance between two points, an equation in which the change of the guide height and the change of the pull-out value of the catenary are unknown is constructed, and the derivative is obtained by solving it. High deltas and pull-out deltas include:

设初始观测时刻为前一观测时刻;Let the initial observation time be the previous observation time;

根据所述主雷达实际坐标、接触网的初始坐标、导高变化量、拉出值变化量、主雷达和接触网之间的初始距离以及当前观测时刻接触网相对于主雷达之间的位移量,构建当前观测时刻主雷达到接触网之间的第一距离方程;According to the actual coordinates of the main radar, the initial coordinates of the catenary, the variation of the guide height, the variation of the pull-out value, the initial distance between the main radar and the catenary, and the displacement of the catenary relative to the main radar at the current observation time , construct the first distance equation between the main radar and the catenary at the current observation moment;

根据所述从雷达实际坐标、接触网的初始坐标、导高变化量、拉出值变化量、从雷达和接触网之间的初始距离以及当前观测时刻接触网相对于从雷达之间的位移量,构建当前观测时刻从雷达到接触网之间的第二距离方程;According to the actual coordinates of the slave radar, the initial coordinates of the catenary, the change of the lead height, the change of the pull-out value, the initial distance between the slave radar and the catenary, and the displacement of the catenary relative to the slave radar at the current observation time , construct the second distance equation between the radar and the catenary at the current observation moment;

分别在多个观测时刻下对所述第一距离方程和第二距离方程进行求解,得到各观测时刻对应的所述导高变化量以及拉出值变化量。The first distance equation and the second distance equation are solved at a plurality of observation times, respectively, to obtain the variation of the lead height and the variation of the pull-out value corresponding to each observation time.

在其中一实施例中,所述根据所述导高变化量以及拉出值变化量进行频谱分析得到所述接触网的力学参数包括:In one of the embodiments, the obtaining of the mechanical parameters of the catenary by performing spectrum analysis according to the variation of the lead height and the variation of the pull-out value includes:

在各观测时刻对应的所述导高变化量以及拉出值变化量中分别寻找出最大导高变化量以及最大拉出值变化量,并根据最大导高变化量以及最大拉出值变化量分别进行计算相应得到导高冲击振幅以及拉出值冲击振幅;The maximum lead height change and the maximum pull value change are respectively found in the lead height change amount and the pull value change amount corresponding to each observation time, and according to the maximum lead height change amount and the maximum pull value change amount respectively Carry out the calculation to obtain the lead-up shock amplitude and the pull-out shock amplitude accordingly;

根据各观测时刻对应的所述导高变化量进行傅里叶变换得到导高变化频谱,并从所述导高变化频谱中提取基频分量,根据所述基频分量以及接触网电缆的张力公式对接触网电缆索的拉力、弦索的线密度以及接触网电缆的等效长度及进行估计得到拉力估计值、线密度估计值以及等效长度估计值。Fourier transform is performed according to the lead height variation corresponding to each observation time to obtain the lead height change spectrum, and the fundamental frequency component is extracted from the lead height change spectrum. According to the fundamental frequency component and the tension formula of the catenary cable The tensile force of the catenary cable, the linear density of the chord cable and the equivalent length of the catenary cable are estimated to obtain the estimated tensile force, linear density and equivalent length.

在其中一实施例中,所述铁路接触网测量方法在根据所述导高变化量以及拉出值变化量进行频谱分析得到所述接触网的力学参数之后还包括:In one embodiment, the method for measuring the railway catenary further includes: after performing spectrum analysis according to the change in the lead height and the change in the pull-out value to obtain the mechanical parameters of the catenary:

根据所述力学参数对接触网进行判断:The catenary is judged according to the mechanical parameters:

若所述力学参数符合预设的设计范围,则判断与观测时刻对应部分的接触网工作正常;If the mechanical parameters meet the preset design range, it is judged that the catenary of the part corresponding to the observation time is working normally;

若所述力学参数不符合预设的设计范围,则判断该部分接触网存在潜在的故障。If the mechanical parameters do not meet the preset design range, it is determined that the part of the catenary has a potential failure.

本申请还提供了一种接触网测量系统,所述接触网测量系统包括相互通信的主雷达、从雷达以及主控装置,所述主雷达和从雷达分别分布在铁路两侧,且两者之间的连线与铁路中心线垂直;The application also provides a catenary measurement system, the catenary measurement system includes a master radar, a slave radar and a master control device that communicate with each other, the master radar and the slave radar are respectively distributed on both sides of the railway, and the other The connection between the lines is perpendicular to the railway centerline;

所述主控装置根据预设的同步方案发送工作指令至所述主雷达和从雷达;The master control device sends work instructions to the master radar and the slave radar according to a preset synchronization scheme;

所述主雷达和从雷达根据所述工作指令向接触网的同一测量点发射测量信号,且将接收到的雷达回波信号发送至所述主控装置;The master radar and the slave radar transmit measurement signals to the same measurement point of the catenary according to the work instruction, and send the received radar echo signals to the master control device;

所述主控装置分别根据主雷达及从雷达发送的初始观测时刻的雷达回波信号进行脉冲压缩得到相应的脉冲压缩图像,且分别识别出接触网在各所述脉冲压缩图像中的波峰位置以及获取所述波峰位置对应的波峰复数散射数据;The main control device performs pulse compression according to the main radar and the radar echo signal at the initial observation time sent from the radar respectively to obtain corresponding pulse compression images, and respectively identifies the peak positions of the catenary in each of the pulse compression images and acquiring the wave peak complex scattering data corresponding to the wave peak position;

从预设的局部坐标系中提取所述主雷达和从雷达的实际坐标,根据各所述实际坐标以及相应的波峰复数散射数据进行计算,得到初始观测时刻所述接触网分别与主雷达和从雷达之间的初始距离,以及所述接触网的初始坐标;The actual coordinates of the main radar and the slave radar are extracted from the preset local coordinate system, and the calculation is performed according to the actual coordinates and the corresponding wave peak complex scattering data to obtain the contact net at the initial observation time. the initial distance between the radars, and the initial coordinates of the catenary;

根据多个观测时刻的雷达回波数据分别得到对应所述主雷达和从雷达的两组复散射观测向量,并根据两组所述复散射观测向量采用时间差分干涉方法得到每一观测时刻所述接触网分别相对于主雷达和从雷达之间的位移量;Two sets of complex scattering observation vectors corresponding to the master radar and the slave radar are obtained according to the radar echo data at multiple observation times, and the time difference interference method is used to obtain the complex scattering observation vectors at each observation time according to the two sets of complex scattering observation vectors. The displacement of the catenary relative to the master radar and the slave radar, respectively;

根据所述主雷达、从雷达的实际坐标、接触网的初始坐标、所述接触网分别与主雷达和从雷达之间的初始距离、以及每一观测时刻所述接触网分别相对于主雷达和从雷达之间的位移量,基于两点间求距离公式构建接触网的导高变化量及拉出值变化量为未知数的方程,并进行求解得到所述导高变化量以及拉出值变化量;According to the actual coordinates of the main radar and the subordinate radar, the initial coordinates of the catenary, the initial distance between the catenary and the main radar and the subordinate radar respectively, and the relative relationship between the catenary and the main radar and the subordinate radar at each observation moment. From the displacement between the radars, based on the formula for finding the distance between two points, construct the equations in which the change of the guide height and the change of the pull-out value of the catenary are unknowns, and solve the equation to obtain the change of the guide height and the change of the pull-out value. ;

根据所述导高变化量以及拉出值变化量进行频谱分析得到所述接触网的力学参数。The mechanical parameters of the catenary are obtained by spectrum analysis according to the variation of the lead height and the variation of the pull-out value.

在其中一实施例中,所述主控装置在根据所述导高变化量以及拉出值变化量进行频谱分析得到所述接触网的力学参数之后还包括:In one embodiment, the main control device further includes: after obtaining the mechanical parameters of the catenary by performing spectrum analysis according to the lead height variation and the pull-out value variation:

根据所述力学参数对接触网进行判断:The catenary is judged according to the mechanical parameters:

若所述力学参数符合预设的设计范围,则判断与观测时刻对应部分的接触网工作正常;If the mechanical parameters meet the preset design range, it is judged that the catenary of the part corresponding to the observation time is working normally;

若所述力学参数不符合预设的设计范围,则判断该部分接触网存在潜在的故障。If the mechanical parameters do not meet the preset design range, it is determined that the part of the catenary has a potential failure.

上述基于雷达系统的铁路接触网测量方法及接触网测量系统,通过在铁路线外两侧分别安装一台雷达,其中一台为主设备雷达(简称主雷达),另一台为从设备雷达(简称从雷达),在主控装置的控制下两个雷达同步工作,采集相同目标在相同时刻不同视角下的雷达回波,并进行脉冲压缩,然后识别接触网在脉冲压缩图像中的波峰位置,接着利用时间差分干涉技术对波峰复数散射数据做干涉处理,分别得到接触网相对于两个雷达的位移量,然后通过求解二元方程得到接触网的导高形变和拉出值形变,最后通过对导高和拉出值的频谱分析估计接触网的力学参数,本方法具有远程非接触、测量精度高、高效实时性强、操作部署便捷等优点。The above-mentioned railway catenary measurement method and catenary measurement system based on radar system, by installing a radar on both sides of the railway line, one of which is the main equipment radar (referred to as the main radar), and the other is the slave equipment radar ( Slave radar for short), under the control of the main control device, the two radars work synchronously, collect radar echoes of the same target at the same time and different viewing angles, and perform pulse compression, and then identify the peak position of the catenary in the pulse compression image, Then, the time difference interference technology is used to interferometrically process the wave peak complex scattering data, and the displacements of the catenary relative to the two radars are obtained respectively. The mechanical parameters of the catenary are estimated by spectral analysis of the lead and pull-out values. This method has the advantages of remote non-contact, high measurement accuracy, high efficiency and real-time performance, and convenient operation and deployment.

附图说明Description of drawings

图1为一个实施例中基于雷达系统的铁路接触网测量方法的流程示意图;1 is a schematic flowchart of a method for measuring a railway catenary based on a radar system in one embodiment;

图2为一个实施例中接触网测量系统的结构示意图;2 is a schematic structural diagram of a catenary measurement system in one embodiment;

图3为一个实施例中铁路接触网受电弓几何模型示意图;3 is a schematic diagram of a geometric model of a railway catenary pantograph in one embodiment;

图4为一个实施例中主、从雷达对接触网测量点进行测量的三维示意图;Fig. 4 is a three-dimensional schematic diagram of the measurement point of the catenary measured by the master and the slave radar in one embodiment;

图5为一个实施例中接触网测量场景的局部坐标示意图。FIG. 5 is a schematic diagram of local coordinates of a catenary measurement scene in one embodiment.

具体实施方式Detailed ways

为了使本申请的目的、技术方案及优点更加清楚明白,以下结合附图及实施例,对本申请进行进一步详细说明。应当理解,此处描述的具体实施例仅仅用以解释本申请,并不用于限定本申请。In order to make the purpose, technical solutions and advantages of the present application more clearly understood, the present application will be described in further detail below with reference to the accompanying drawings and embodiments. It should be understood that the specific embodiments described herein are only used to explain the present application, but not to limit the present application.

如图1-2所示,提供了一种基于雷达系统的铁路接触网测量方法,该方法应用于接触网测量系统,接触网测量系统包括相互通信的主雷达、从雷达以及主控装置,主雷达和从雷达分别分布在铁路两侧,且两者之间的连线与铁路中心线垂直。As shown in Figure 1-2, a radar system-based railway catenary measurement method is provided. The method is applied to the catenary measurement system. The catenary measurement system includes a master radar, a slave radar and a master control device that communicate with each other. The radar and the slave radar are distributed on both sides of the railway, and the connection between the two is perpendicular to the center line of the railway.

铁路接触网测量方法具体包括以下步骤:The railway catenary measurement method specifically includes the following steps:

步骤S100,主控装置根据预设的同步方案发送工作指令至主雷达和从雷达;Step S100, the master control device sends a work instruction to the master radar and the slave radar according to a preset synchronization scheme;

步骤S110,主雷达和从雷达根据工作指令向接触网的同一测量点发射测量信号,且将接收到的雷达回波信号发送至主控装置;Step S110, the master radar and the slave radar transmit measurement signals to the same measurement point of the catenary according to the work instruction, and send the received radar echo signals to the master control device;

步骤S120,主控装置分别根据主雷达及从雷达发送的初始观测时刻的雷达回波信号进行脉冲压缩得到相应的脉冲压缩图像,且分别识别出接触网在各脉冲压缩图像中的波峰位置,以及获取所述波峰位置对应的波峰复数散射数据;Step S120, the main control device performs pulse compression according to the radar echo signal at the initial observation time sent by the main radar and the slave radar respectively to obtain corresponding pulse compression images, and respectively identifies the peak positions of the catenary in each pulse compression image, and acquiring the wave peak complex scattering data corresponding to the wave peak position;

步骤S130,从预设的局部坐标系中提取主雷达和从雷达的实际坐标,根据各实际坐标以及相应的波峰复数散射数据进行计算,得到初始观测时刻接触网分别与主雷达和从雷达之间的初始距离以及所述接触网的初始坐标;Step S130, extracting the actual coordinates of the main radar and the subordinate radar from the preset local coordinate system, and calculating according to the actual coordinates and the corresponding peak complex scattering data to obtain the difference between the catenary and the main radar and the subordinate radar at the initial observation time. The initial distance of and the initial coordinates of the catenary;

步骤S140,根据多个观测时刻的雷达回波数据分别得到对应主雷达和从雷达的两组复散射观测向量,并根据两组复散射观测向量采用时间差分干涉方法得到每一观测时刻接触网分别相对于主雷达和从雷达之间的位移量;In step S140, two sets of complex scattering observation vectors corresponding to the main radar and the slave radar are obtained according to the radar echo data at multiple observation times, and a time difference interference method is used to obtain the catenary at each observation time according to the two sets of complex scattering observation vectors. relative to the displacement between the master radar and the slave radar;

步骤S150,根据所述主雷达、从雷达的实际坐标、接触网的初始坐标、所述接触网分别与主雷达和从雷达之间的初始距离、以及每一观测时刻所述接触网分别相对于主雷达和从雷达之间的位移量,基于两点间求距离公式构建接触网的导高变化量及拉出值变化量为未知数的方程,并进行求解得到导高变化量以及拉出值变化量;Step S150, according to the actual coordinates of the main radar and the subordinate radar, the initial coordinates of the catenary, the initial distance between the catenary and the main radar and the subordinate radar respectively, and the relative position of the catenary at each observation moment. The displacement between the master radar and the slave radar is based on the formula for finding the distance between two points to construct the equations of the change of the lead height and the change of the pull-out value of the catenary as unknowns, and solve it to obtain the change of the lead-to-height and the change of the pull-out value. quantity;

步骤S160,根据导高变化量以及拉出值变化量进行频谱分析得到接触网的力学参数。In step S160, the mechanical parameters of the catenary are obtained by spectrum analysis according to the variation of the lead height and the variation of the pull-out value.

本申请提供了一种用于如图3所示的铁路接触网场景中的接触网测量方法,用于对接触网的各关键技术指标进行实时动态遥测,其中关键技术指标包括接触线导高、拉出值等几何参数,接触网拉力、动态振幅等力学参数。The present application provides a catenary measurement method used in a railway catenary scenario as shown in FIG. 3 , which is used to perform real-time dynamic telemetry on various key technical indicators of the catenary, wherein the key technical indicators include contact wire conductance, Geometric parameters such as pull-out value, mechanical parameters such as catenary tension, dynamic amplitude, etc.

在本实施例中,该铁路接触网测量方法应用于一接触网测量系统中,该接触网测量系统是由雷达作为对接触网进行测量的主体,并且在主控装置中对雷达回波信号进行相应处理后得到当前时刻下接触网各关键技术指标,以实现对铁路接触网实时状态进行检测的目的。In this embodiment, the railway catenary measurement method is applied to a catenary measurement system. The catenary measurement system uses radar as the main body to measure the catenary, and the radar echo signal is measured in the main control device. After corresponding processing, the key technical indicators of the catenary at the current moment are obtained, so as to realize the purpose of detecting the real-time status of the railway catenary.

在本实施例中,主控装置可为上位机。In this embodiment, the main control device may be an upper computer.

在本实施例中,接触网测量系统包括分别布置在铁路线外侧的两部雷达,其中一部作为主雷达,另外一部作为从雷达。在对两雷达进行现场布置时,确保雷达与被观测的接触网电缆之间没有遮挡,调整雷达天线波束指向,使雷达波束中心对准接触网电缆。In this embodiment, the catenary measurement system includes two radars respectively arranged outside the railway line, one of which is used as the main radar, and the other is used as the slave radar. When arranging the two radars on site, make sure that there is no obstruction between the radar and the catenary cable being observed, and adjust the radar antenna beam direction so that the center of the radar beam is aligned with the catenary cable.

为了提高接触网测量精度,且在条件允许方位内,应控制两部雷达的直线距离尽量大。在一些实施例中,两部雷达之间的距离可在10米左右。In order to improve the measurement accuracy of the catenary, and within the allowable azimuth, the straight-line distance between the two radars should be controlled as large as possible. In some embodiments, the distance between the two radars may be around 10 meters.

并且,根据雷达原理,接触网长电缆在测量点的法平面上散射最强,还需要进一步控制两部雷达位置,使得两者连线AB与接触网电缆垂直,如图4所示。Moreover, according to the radar principle, the long catenary cable has the strongest scattering on the normal plane of the measurement point, and it is necessary to further control the positions of the two radars so that the connecting line AB of the two is perpendicular to the catenary cable, as shown in Figure 4.

在步骤S100-S110中,为主控装置向两部雷达分别发送工作指令,以使两部雷达根据工作指令向同一接触网的测量点发射测量信号,再将接收到的雷达回波信号发送至主控装置。之后在主控装置内对分别接收到的雷达回波数据进行处理。In steps S100-S110, the main control device sends work instructions to the two radars respectively, so that the two radars transmit measurement signals to the measurement points of the same catenary according to the work instructions, and then send the received radar echo signals to the master device. Afterwards, the respectively received radar echo data are processed in the main control device.

由于接触网距离主、从雷达较近,因此两部雷达应当采用宽带相参连续波体制,这两部雷达与常规超近程雷达和一维形变测量雷达结构相似。雷达在主控装置的控制下同步工作。为了防止两部雷达产生同频干扰影响测量精度,可通过主控装置发送相应的工作指令使其在两种不同的同步方案下进行测量工作。Since the catenary is relatively close to the master and slave radars, the two radars should adopt the broadband coherent continuous wave system. The two radars are similar in structure to the conventional ultra-short-range radar and the one-dimensional deformation measurement radar. The radar works synchronously under the control of the main control device. In order to prevent the co-frequency interference of the two radars from affecting the measurement accuracy, the main control device can send corresponding work instructions to make the measurement work under two different synchronization schemes.

在本实施例中,预设的同步方案包括第一同步方案和第二同步方案。In this embodiment, the preset synchronization scheme includes a first synchronization scheme and a second synchronization scheme.

其中,第一同步方案包括控制主雷达和从雷达在相同时刻发射波形为不同频率或不同编码的测量信号。The first synchronization scheme includes controlling the master radar and the slave radar to transmit measurement signals with waveforms of different frequencies or different codes at the same time.

具体的,主、从两部雷达的发射波形可以从频率或者编码方式上进行区分,主控装置通过指令控制两部雷达工作在不同频率上,或者采用不同的编码发射波形,而两部雷达以相同的脉冲重复频率进行测量。Specifically, the transmission waveforms of the master and slave radars can be distinguished in terms of frequency or coding method. The master control device controls the two radars to work on different frequencies through instructions, or uses different coding transmission waveforms, while the two radars use The same pulse repetition frequency was measured.

进一步的,可由主雷达产生测量时序并传输至从雷达,使得两者工作于相同的测量时序。也可以由两部雷达独立产生时序,在各自的时序下进行工作,然后将测量的雷达回波信号上打上采样时刻标志,最后在主控装置上进行数据时间配准。Further, the measurement sequence can be generated by the master radar and transmitted to the slave radar, so that both work in the same measurement sequence. Alternatively, two radars can independently generate time sequences, work under their respective time sequences, and then mark the measured radar echo signals with sampling time marks, and finally perform data time registration on the main control device.

其中,第二同步方案包括控制主雷达和从雷达交替发射波形为相同频率和相同编码的测量信号。Wherein, the second synchronization scheme includes controlling the master radar and the slave radar to alternately transmit measurement signals whose waveforms are the same frequency and the same code.

具体的,当两部雷达工作频率和编码方式相同时,可以通过分时工作的方式避免相互干扰。其中测量时序由主雷达产生,通过有线或无线信道,将工作时序传输至从雷达,通过时序设计使得主从雷达交替工作,避免干扰。Specifically, when the working frequencies and coding methods of the two radars are the same, mutual interference can be avoided by working in a time-sharing manner. The measurement sequence is generated by the master radar, and the working sequence is transmitted to the slave radar through wired or wireless channels. Through the timing design, the master and slave radars work alternately to avoid interference.

在本实施例中,主雷达和从雷达发射的测量信号带宽大于500MHz。In this embodiment, the bandwidth of the measurement signal transmitted by the master radar and the slave radar is greater than 500 MHz.

根据《铁路电力牵引供电设计规范》,承力拉索到接触网电缆的吊弦长度最短约为0.3米,因此两部雷达的距离分辨率应当优于0.3米,根据雷达原理可知:两部雷达的发射信号带宽应当大于500MHz,否则将不能有效区分接触网上下两根线缆。According to the "Code for Design of Railway Electric Traction Power Supply", the shortest chord length from the load-bearing cable to the catenary cable is about 0.3 meters, so the distance resolution of the two radars should be better than 0.3 meters. The bandwidth of the transmitted signal should be greater than 500MHz, otherwise it will not be able to effectively distinguish between the two cables on the contact line.

主雷达以及从雷达接收到工作指令后向接触网以一定的脉冲重复频率发射测量信号,在此过程中在火车的运动下接触网上的测量点也会发生一定的位移,所以接收到的雷达回波数据包括有不同观测时刻的关于接触网上同一测量点的多个信号数据。而通过接收到的初始雷达回波数据可以确定初始时刻两雷达分别与接触网的距离,以及接触网的初始位置。The main radar and the slave radar transmit measurement signals to the catenary at a certain pulse repetition frequency after receiving the work order. The wave data includes multiple signal data about the same measurement point on the catenary at different observation times. The distance between the two radars and the catenary and the initial position of the catenary can be determined through the received initial radar echo data.

在步骤S120中,主控装置首先通过分别从主雷达和从雷达处接收到的雷达回波数据进行脉冲压缩。其中,主、从雷达可采用宽带雷达信号包括步进频率信号、相位编码信号和线性调频信号,以线性调频信号为例,两部雷达发射的雷达回波信号可表示为:In step S120, the main control device first performs pulse compression on the radar echo data received from the main radar and the slave radar respectively. Among them, the master and slave radars can use broadband radar signals including step frequency signals, phase encoded signals and chirp signals. Taking chirp signals as an example, the radar echo signals emitted by the two radars can be expressed as:

Figure 884969DEST_PATH_IMAGE001
(1)
Figure 884969DEST_PATH_IMAGE001
(1)

在公式(1)中,

Figure 72368DEST_PATH_IMAGE002
为脉冲内快采样时间,
Figure 480478DEST_PATH_IMAGE003
为起始频率,
Figure 55816DEST_PATH_IMAGE004
为线性调频扫频周期,
Figure 595382DEST_PATH_IMAGE005
为调频斜率,
Figure 117630DEST_PATH_IMAGE006
是虚数单位,
Figure 409940DEST_PATH_IMAGE007
为发射信号幅度,对形变估计的影响较小,在后续表达式中将其省略,矩形函数
Figure 359441DEST_PATH_IMAGE008
。In formula (1),
Figure 72368DEST_PATH_IMAGE002
is the fast sampling time within the pulse,
Figure 480478DEST_PATH_IMAGE003
is the starting frequency,
Figure 55816DEST_PATH_IMAGE004
is the chirp frequency sweep period,
Figure 595382DEST_PATH_IMAGE005
is the frequency modulation slope,
Figure 117630DEST_PATH_IMAGE006
is an imaginary unit,
Figure 409940DEST_PATH_IMAGE007
is the amplitude of the transmitted signal, which has little influence on the deformation estimation, and is omitted in the subsequent expressions. The rectangular function
Figure 359441DEST_PATH_IMAGE008
.

在本实施例中,在对雷达回波信号进行脉冲压缩处理前,对其进行去调频接收后,接收输出固定频率的中频回波,该中频回波的频率大小与接触网到雷达的距离成正比,再经过AD模数转换采集装置的处理后得到数字雷达回波信号。最后对处理后的雷达回波信号进行脉冲压缩,脉冲压缩的结果为:In this embodiment, before pulse compression processing is performed on the radar echo signal, after it is received by frequency modulation, an intermediate frequency echo of a fixed frequency is received and output, and the frequency of the intermediate frequency echo is proportional to the distance from the catenary to the radar. Proportional to the digital radar echo signal after processing by the AD analog-to-digital conversion acquisition device. Finally, pulse compression is performed on the processed radar echo signal, and the result of pulse compression is:

Figure 120724DEST_PATH_IMAGE009
(2)
Figure 120724DEST_PATH_IMAGE009
(2)

在公式(2)中,

Figure 446663DEST_PATH_IMAGE010
表示FFT的长度,
Figure 406529DEST_PATH_IMAGE011
表示中频回波的AD采样频率,
Figure 277664DEST_PATH_IMAGE012
表示中频回波的AD采样点数。其中
Figure 526243DEST_PATH_IMAGE013
表示电磁波从发射,照射到接触网电缆,最后再被雷达接收的双程传输延迟,假设接触网电缆的位置坐标为
Figure 390293DEST_PATH_IMAGE014
,则接触网在主雷达的延迟为:
Figure 407928DEST_PATH_IMAGE015
,接触网在从雷达中的延迟为:
Figure 761549DEST_PATH_IMAGE016
。In formula (2),
Figure 446663DEST_PATH_IMAGE010
represents the length of the FFT,
Figure 406529DEST_PATH_IMAGE011
Indicates the AD sampling frequency of the IF echo,
Figure 277664DEST_PATH_IMAGE012
Indicates the AD sampling points of the IF echo. in
Figure 526243DEST_PATH_IMAGE013
Represents the two-way transmission delay of the electromagnetic wave from the launch, irradiation to the catenary cable, and finally being received by the radar. It is assumed that the position coordinates of the catenary cable are
Figure 390293DEST_PATH_IMAGE014
, then the delay of the catenary in the main radar is:
Figure 407928DEST_PATH_IMAGE015
, the delay of the catenary in the slave radar is:
Figure 761549DEST_PATH_IMAGE016
.

其中,

Figure 481112DEST_PATH_IMAGE017
为主雷达的坐标,
Figure 680012DEST_PATH_IMAGE018
为从雷达的坐标。in,
Figure 481112DEST_PATH_IMAGE017
are the coordinates of the primary radar,
Figure 680012DEST_PATH_IMAGE018
for the coordinates from the radar.

经过脉冲压缩后:在主雷达中,接触网的脉冲压缩波峰位于

Figure 817733DEST_PATH_IMAGE019
;在从雷达中,接触网的脉冲压缩波峰位于
Figure 279938DEST_PATH_IMAGE020
;其中,
Figure 237530DEST_PATH_IMAGE021
表示四舍五入取整运算。After pulse compression: In the main radar, the pulse compression peak of the catenary is at
Figure 817733DEST_PATH_IMAGE019
; in the slave radar, the pulse-compression peak of the catenary is located at
Figure 279938DEST_PATH_IMAGE020
;in,
Figure 237530DEST_PATH_IMAGE021
Indicates the rounding operation.

而峰值处对应的复数散射值分别记为:

Figure 477273DEST_PATH_IMAGE022
Figure 469500DEST_PATH_IMAGE023
,其相位分别为
Figure 899344DEST_PATH_IMAGE024
Figure 609811DEST_PATH_IMAGE025
,由于其中的第二项远小于第一项,因此该相位可分别近似为
Figure 353776DEST_PATH_IMAGE026
Figure 997247DEST_PATH_IMAGE027
。The complex scattering values corresponding to the peaks are denoted as:
Figure 477273DEST_PATH_IMAGE022
and
Figure 469500DEST_PATH_IMAGE023
, whose phases are
Figure 899344DEST_PATH_IMAGE024
and
Figure 609811DEST_PATH_IMAGE025
, since the second term is much smaller than the first term, the phases can be respectively approximated as
Figure 353776DEST_PATH_IMAGE026
and
Figure 997247DEST_PATH_IMAGE027
.

在其他实施例中,对雷达回波数据进行脉冲压缩处理还可以是在主雷达、从雷达本地完成,再将脉冲压缩的结果发送至主控装置中进行后续计算,则对应步骤S110至步骤S120中调整为:In other embodiments, the pulse compression processing on the radar echo data may also be performed locally on the master radar and the slave radar, and then the pulse compression result is sent to the master control device for subsequent calculation, corresponding to steps S110 to S120 Adjusted to:

步骤S110,主雷达和从雷达根据所工作指令向接触网的同一测量点发射测量信号,接收到的雷达回波信号后,分别对雷达回波信号进行脉冲压缩得到压缩后的雷达回波信号,并将其发送至主控装置;Step S110, the master radar and the slave radar transmit measurement signals to the same measurement point of the catenary according to the working instructions, and after receiving the radar echo signals, pulse-compress the radar echo signals respectively to obtain the compressed radar echo signals, and send it to the master device;

步骤S120中,主控装置根据主雷达及从雷达发送的初始观测时刻的压缩后的雷达回波信号,并将其转换成脉冲压缩图像,识别出接触网在各所述脉冲压缩图像中的波峰位置、以及获取所述波峰位置对应的波峰复数散射数据。In step S120, the main control device converts the compressed radar echo signal at the initial observation time sent by the main radar and the slave radar into a pulse-compressed image, and identifies the peaks of the catenary in each of the pulse-compressed images. position, and obtain the wave peak complex scattering data corresponding to the wave peak position.

在对各雷达回波数据进行脉冲压缩处理后得到各脉冲压缩图像中的波峰复数散射数据,再利用该数据以及主、从雷达的坐标位置对初始观测时刻接触网分别与主雷达和从雷达之间的初始距离。After pulse compression processing is performed on the echo data of each radar, the peak complex scattering data in each pulse compressed image is obtained, and then the data and the coordinate positions of the master and slave radars are used to analyze the relationship between the catenary and the master radar and the slave radar respectively at the initial observation time. initial distance between.

在步骤S130中,如图5所示,建立局部坐标系

Figure 316102DEST_PATH_IMAGE028
,坐标面由两个雷达和接触网测量点构成,坐标原点为铁路路面中心,y轴方向为垂直向上方向,x轴方向为接触网电缆垂直方向,通过定位设备(如差分北斗/GPS,全站仪等)测量主雷达的实际坐标值
Figure 982706DEST_PATH_IMAGE029
和从雷达的实际坐标值
Figure 795942DEST_PATH_IMAGE030
。In step S130, as shown in FIG. 5, a local coordinate system is established
Figure 316102DEST_PATH_IMAGE028
, the coordinate plane is composed of two radar and catenary measurement points, the coordinate origin is the center of the railway road, the y -axis direction is the vertical upward direction, and the x -axis direction is the vertical direction of the catenary cable. station, etc.) to measure the actual coordinate value of the main radar
Figure 982706DEST_PATH_IMAGE029
and the actual coordinate values from the radar
Figure 795942DEST_PATH_IMAGE030
.

则根据脉冲压缩波峰位置下标和雷达系统参数可以得到初始时刻接触网电缆到主雷达的距离为

Figure 559498DEST_PATH_IMAGE031
,初始时刻接触网络到从雷达的距离为
Figure 268828DEST_PATH_IMAGE032
。Then, according to the subscript of the pulse compression peak position and the radar system parameters, the distance from the catenary cable to the main radar at the initial moment can be obtained as:
Figure 559498DEST_PATH_IMAGE031
, the distance from the contact network to the radar at the initial moment is
Figure 268828DEST_PATH_IMAGE032
.

在得到初始观测时刻所述接触网分别与主雷达和从雷达之间的初始距离之后包括:After obtaining the initial distances between the catenary and the primary radar and the secondary radar respectively at the initial observation time, it includes:

根据主雷达实际坐标、主雷达与接触网之间的初始距离构建接触网的初始坐标为未知数的第一方程;According to the actual coordinates of the main radar and the initial distance between the main radar and the catenary, construct the first equation in which the initial coordinates of the catenary are unknowns;

根据从雷达实际坐标、从雷达与接触网之间的初始距离构建接触网的初始坐标为未知数的第二方程;According to the actual coordinates of the radar and the initial distance between the radar and the catenary, a second equation with the initial coordinates of the catenary as an unknown number is constructed;

利用第一方程和第二方程进行求解,得到所述接触网的初始坐标。Solve the first equation and the second equation to obtain the initial coordinates of the catenary.

具体的,第一方程和第二方程可得到下属方程组:Specifically, the first equation and the second equation can obtain the following equations:

Figure 704620DEST_PATH_IMAGE033
(3)
Figure 704620DEST_PATH_IMAGE033
(3)

在公式(3)中,由于主雷达实际坐标、主雷达与接触网之间的初始距离、从雷达实际坐标、从雷达与接触网之间的初始距离均为已知数,则可对公式(3)进行求解得到初始观测时刻接触网的坐标值也就是接触网的初始位置。In formula (3), since the actual coordinates of the main radar, the initial distance between the main radar and the catenary, the actual coordinates of the secondary radar, and the initial distance between the secondary radar and the catenary are all known numbers, the formula ( 3) Solve to obtain the coordinate value of the catenary at the initial observation time, that is, the initial position of the catenary.

在步骤S140中,由于在对接触网进行测量时,会得到对应不同时刻的多个雷达回波数据,可以对各雷达回波数据进行脉冲压缩处理得到两组分别对应主雷达和从雷达的复散射观测向量。In step S140, since a plurality of radar echo data corresponding to different times will be obtained when the catenary is measured, pulse compression processing can be performed on each radar echo data to obtain two sets of complex data corresponding to the master radar and the slave radar respectively. Scatter observation vector.

具体的,假设两部雷达重复测量频率为

Figure 852705DEST_PATH_IMAGE034
,在不同
Figure 674030DEST_PATH_IMAGE035
时刻可以获得主雷达关于接触网电缆的一组复散射观测向量
Figure 554261DEST_PATH_IMAGE036
,以及从雷达关于接触网电缆的一组复散射观测向量
Figure 461037DEST_PATH_IMAGE037
。Specifically, it is assumed that the repeated measurement frequency of the two radars is
Figure 852705DEST_PATH_IMAGE034
,in difference
Figure 674030DEST_PATH_IMAGE035
A set of complex scattering observation vectors of the main radar about the catenary cable can be obtained at the moment
Figure 554261DEST_PATH_IMAGE036
, and a set of complex scattering observation vectors from radar on catenary cables
Figure 461037DEST_PATH_IMAGE037
.

再利用时间差分干涉原理估计接触网电缆相对于初始位置的径向形变量,也就是接触网分别相对于主雷达和从雷达之间的位移量。Then, the time difference interference principle is used to estimate the radial deformation of the catenary cable relative to the initial position, that is, the displacement of the catenary relative to the master radar and the slave radar respectively.

其中,每一观测时刻接触网电缆相对于主雷达的位移量为:

Figure 412813DEST_PATH_IMAGE038
。Among them, the displacement of the catenary cable relative to the main radar at each observation moment is:
Figure 412813DEST_PATH_IMAGE038
.

其中,每一观测时刻接触网电缆相对于从雷达的位移量为:

Figure 337912DEST_PATH_IMAGE039
。Among them, the displacement of the catenary cable relative to the slave radar at each observation moment is:
Figure 337912DEST_PATH_IMAGE039
.

如图5所示,其中点A为接触网在初始观测时刻tn所在的初始位置,且设初始位置为上一观测时刻,则点B为接触网在当下观测时刻tn+1所在的当前位置。由于接触网的位移是通过在Y轴方向上的导高变化量和X轴方向上的拉出值变化量导致的,则可以根据接触网在初始位置上时,分别与主雷达和从雷达之间的距离公式推出接触网在当前位置上时,分别与主雷达和从雷达之间的位置公式,并将导高变化量以及拉出值变化量作为未知量进行求解。As shown in Figure 5, where point A is the initial position of the catenary at the initial observation time t n , and the initial position is the previous observation time, then point B is the current position of the catenary at the current observation time t n+1 Location. Since the displacement of the catenary is caused by the change of the lead height in the Y-axis direction and the change of the pull-out value in the X-axis direction, it can be compared with the main radar and the slave radar respectively according to the initial position of the catenary. When the catenary is at the current position, the position formula between the main radar and the slave radar is derived from the formula of the distance between them, and the variation of the lead height and the variation of the pull-out value are solved as unknown quantities.

其中,根据主雷达实际坐标、接触网的初始坐标、导高变化量、拉出值变化量、主雷达和接触网之间的初始距离以及当前观测时刻接触网相对于主雷达之间的位移量,构建当前观测时刻主雷达到接触网之间的第一距离方程;Among them, according to the actual coordinates of the main radar, the initial coordinates of the catenary, the change of the guide height, the change of the pull-out value, the initial distance between the main radar and the catenary, and the displacement of the catenary relative to the main radar at the current observation time , construct the first distance equation between the main radar and the catenary at the current observation moment;

其中,根据从雷达实际坐标、接触网的初始坐标、导高变化量、拉出值变化量、从雷达和接触网之间的初始距离以及当前观测时刻接触网相对于从雷达之间的位移量,构建当前观测时刻从雷达到接触网之间的第二距离方程。Among them, according to the actual coordinates of the slave radar, the initial coordinates of the catenary, the variation of the guide height, the change of the pull-out value, the initial distance between the slave radar and the catenary, and the displacement of the catenary relative to the slave radar at the current observation time , and construct the second distance equation between the radar and the catenary at the current observation moment.

由第一距离方程和第二距离方程进行组合得到:It is obtained by combining the first distance equation and the second distance equation:

Figure 654624DEST_PATH_IMAGE040
(4)
Figure 654624DEST_PATH_IMAGE040
(4)

在公式(4)中,

Figure 845434DEST_PATH_IMAGE041
为公式(3)的解,也就是接触网在初始位置的坐标,
Figure 538584DEST_PATH_IMAGE042
Figure 68922DEST_PATH_IMAGE043
分别为导高变化量以及拉出值变化量,而
Figure 572847DEST_PATH_IMAGE044
Figure 188636DEST_PATH_IMAGE045
为两个雷达的观测距离存在的位移变化量。而公式(4)中两方程的右边实际就是图5中
Figure 482214DEST_PATH_IMAGE046
Figure 132638DEST_PATH_IMAGE047
的值。In formula (4),
Figure 845434DEST_PATH_IMAGE041
is the solution of formula (3), that is, the coordinates of the catenary at the initial position,
Figure 538584DEST_PATH_IMAGE042
and
Figure 68922DEST_PATH_IMAGE043
are the variation of the lead height and the variation of the pull-out value, respectively, and
Figure 572847DEST_PATH_IMAGE044
and
Figure 188636DEST_PATH_IMAGE045
It is the displacement variation that exists between the observation distances of the two radars. The right side of the two equations in formula (4) is actually in Figure 5
Figure 482214DEST_PATH_IMAGE046
and
Figure 132638DEST_PATH_IMAGE047
value of .

分别在多个观测时刻下对第一距离方程和第二距离方程进行求解,得到各观测时刻对应的导高变化量以及拉出值变化量。The first distance equation and the second distance equation are solved at multiple observation times respectively, and the variation of the lead height and the variation of the pull-out value corresponding to each observation moment are obtained.

具体的,在其他时刻

Figure 791153DEST_PATH_IMAGE048
,接触网相对于初始位置
Figure 956555DEST_PATH_IMAGE049
,导高和拉出值分别存在变量。Specifically, at other times
Figure 791153DEST_PATH_IMAGE048
, the catenary relative to the initial position
Figure 956555DEST_PATH_IMAGE049
, and there are variables for the lead-up and pull-out values, respectively.

在对公式(4)中的导高变量和拉出值变量进行求解时,将公式(4)与公式(3)两个方程组进行相减,得到新的方程组:When solving the lead-up variable and the pull-out value variable in formula (4), the two equations of formula (4) and formula (3) are subtracted to obtain a new set of equations:

Figure 240775DEST_PATH_IMAGE050
(5)
Figure 240775DEST_PATH_IMAGE050
(5)

在公式(5)中,由于导高变化量

Figure 480126DEST_PATH_IMAGE051
和拉出值变化量
Figure 575121DEST_PATH_IMAGE052
较小,可知方程组左边第二项和第四项分别小于第一项和第三项,方程组右边第二项远小于第一项,因此该方程组简化为:In Equation (5), due to the lead change
Figure 480126DEST_PATH_IMAGE051
and pull-out value change
Figure 575121DEST_PATH_IMAGE052
It can be seen that the second term and fourth term on the left side of the equation system are smaller than the first term and the third term respectively, and the second term on the right side of the equation system is much smaller than the first term, so the equation system is simplified as:

Figure 962240DEST_PATH_IMAGE053
(6)
Figure 962240DEST_PATH_IMAGE053
(6)

根据公式(6),可以得到导高变化和拉出值变化的估计分别为:According to formula (6), the estimates of the change of lead height and the change of pull-out value can be obtained as:

Figure 535304DEST_PATH_IMAGE054
(7)
Figure 535304DEST_PATH_IMAGE054
(7)

根据公式(7),可求解出各观测时刻对应的导高变化和拉出值变化。According to formula (7), the change of lead height and the change of pull-out value corresponding to each observation time can be solved.

在步骤S160中,根据导高变化量以及拉出值变化量进行频谱分析得到接触网的力学参数包括:在各观测时刻对应的导高变化量以及拉出值变化量中分别寻找出最大导高变化量以及最大拉出值变化量,并根据最大导高变化量以及最大拉出值变化量分别进行计算相应得到导高冲击振幅(上下抬升量)

Figure 911053DEST_PATH_IMAGE055
以及拉出值冲击振幅(左右摆动量)
Figure 973687DEST_PATH_IMAGE056
。In step S160 , the mechanical parameters of the catenary obtained by spectrum analysis according to the variation of the lead height and the change of the pull-out value include: finding the maximum lead-height among the changes of the lead-up height and the change of the pull-out value corresponding to each observation time. The change amount and the maximum pull-out value change amount, and according to the maximum lead-up value change amount and the maximum pull-out value change amount, respectively, the lead-up impact amplitude (up and down lift) is calculated accordingly.
Figure 911053DEST_PATH_IMAGE055
And the pull-out value shock amplitude (left-right swing amount)
Figure 973687DEST_PATH_IMAGE056
.

其中,

Figure 51364DEST_PATH_IMAGE057
以及
Figure 428119DEST_PATH_IMAGE058
分别为:in,
Figure 51364DEST_PATH_IMAGE057
as well as
Figure 428119DEST_PATH_IMAGE058
They are:

Figure 907642DEST_PATH_IMAGE059
(8)
Figure 907642DEST_PATH_IMAGE059
(8)

根据各观测时刻对应的导高变化量进行傅里叶变换得到导高变化频谱,并从所述导高变化频谱中提取基频分量,根据基频分量以及接触网电缆的张力公式对接触网电缆索的拉力、弦索的线密度以及接触网电缆的等效长度及进行估计得到拉力估计值、线密度估计值以及等效长度估计值。Fourier transform is performed on the lead height variation corresponding to each observation time to obtain the lead height change spectrum, and the fundamental frequency component is extracted from the lead height change spectrum. According to the fundamental frequency component and the tension formula of the catenary cable, the catenary cable is The tensile force of the cable, the linear density of the string cable and the equivalent length of the catenary cable are estimated to obtain the estimated tensile force, linear density and equivalent length.

其中,基频分量为

Figure 328128DEST_PATH_IMAGE060
,张力
Figure 689839DEST_PATH_IMAGE061
可按照公式
Figure 870284DEST_PATH_IMAGE062
。其中, q是弦索的线密度,
Figure 204314DEST_PATH_IMAGE063
表示接触网电缆的等效长度。Among them, the fundamental frequency component is
Figure 328128DEST_PATH_IMAGE060
,tension
Figure 689839DEST_PATH_IMAGE061
according to the formula
Figure 870284DEST_PATH_IMAGE062
. where q is the linear density of the string,
Figure 204314DEST_PATH_IMAGE063
Indicates the equivalent length of the catenary cable.

在本实施例中,铁路接触网测量方法在根据所述导高变化量以及拉出值变化量进行频谱分析得到接触网的力学参数之后还包括:In this embodiment, the method for measuring the railway catenary further includes: after performing spectrum analysis according to the variation of the lead height and the variation of the pull-out value to obtain the mechanical parameters of the catenary:

根据力学参数对接触网进行判断:The catenary is judged according to the mechanical parameters:

若力学参数符合预设的设计范围,则判断与观测时刻对应部分的接触网工作正常;If the mechanical parameters conform to the preset design range, it is judged that the catenary of the part corresponding to the observation time is working normally;

若力学参数不符合预设的设计范围,则判断该部分接触网存在潜在的故障。If the mechanical parameters do not meet the preset design range, it is judged that this part of the catenary has potential failures.

上述基于雷达系统的铁路接触网测量方法中,在铁路线外两侧分别安装一台雷达,其中一台为主设备雷达(简称主雷达),另一台为从设备雷达(从雷达),在主控计算机或主雷达的控制下两个雷达同步工作,采集相同目标在相同时刻不同视角下的雷达回波,并进行脉冲压缩,然后识别接触网在脉冲压缩图像中的波峰位置,接着利用时间差分干涉技术对波峰复数散射数据做干涉处理,分别得到接触网相对于两个雷达的位移量,然后通过求解二元方程得到接触网的导高形变和拉出值形变,最后通过对导高和拉出值的频谱分析估计接触网的力学参数,判断接触网的健康状况。本方法具有远程非接触、测量精度高、高效实时性强、操作部署便捷等优点。且对列车运行无影响,环境适应性优良。可广泛用于对常规铁路、高速铁路的接触网进行实时监测,保障铁路运行安全,也可用于为下一代高速铁路设计和相关标准确立提供科研技术支撑。In the above railway catenary measurement method based on radar system, one radar is installed on both sides of the railway line, one of which is the main equipment radar (referred to as the main radar), and the other is the slave equipment radar (slave radar). The two radars work synchronously under the control of the main control computer or the main radar, collect the radar echoes of the same target at the same time and different viewing angles, and perform pulse compression, and then identify the peak position of the catenary in the pulse compression image, and then use the time The differential interferometric technique interferometrically processes the complex scattering data of the wave peaks, and obtains the displacement of the catenary relative to the two radars, respectively, and then obtains the guide height deformation and the pull-out value deformation of the catenary by solving the binary equation. Spectral analysis of pull-out values estimates the mechanical parameters of the catenary and judges the health of the catenary. The method has the advantages of remote non-contact, high measurement accuracy, high efficiency and real-time performance, and convenient operation and deployment. And it has no impact on train operation, and has excellent environmental adaptability. It can be widely used for real-time monitoring of the catenary of conventional railways and high-speed railways to ensure the safety of railway operation, and can also be used to provide scientific research and technical support for the design of the next generation of high-speed railways and the establishment of relevant standards.

应该理解的是,虽然图1的流程图中的各个步骤按照箭头的指示依次显示,但是这些步骤并不是必然按照箭头指示的顺序依次执行。除非本文中有明确的说明,这些步骤的执行并没有严格的顺序限制,这些步骤可以以其它的顺序执行。而且,图1中的至少一部分步骤可以包括多个子步骤或者多个阶段,这些子步骤或者阶段并不必然是在同一时刻执行完成,而是可以在不同的时刻执行,这些子步骤或者阶段的执行顺序也不必然是依次进行,而是可以与其它步骤或者其它步骤的子步骤或者阶段的至少一部分轮流或者交替地执行。It should be understood that although the various steps in the flowchart of FIG. 1 are shown in sequence according to the arrows, these steps are not necessarily executed in the sequence shown by the arrows. Unless explicitly stated herein, the execution of these steps is not strictly limited to the order, and these steps may be performed in other orders. Moreover, at least a part of the steps in FIG. 1 may include multiple sub-steps or multiple stages. These sub-steps or stages are not necessarily executed and completed at the same time, but may be executed at different times. The execution of these sub-steps or stages The sequence is also not necessarily sequential, but may be performed alternately or alternately with other steps or sub-steps of other steps or at least a portion of a phase.

在一个实施例中,提供了一种接触网测量系统,所述接触网测量系统包括相互通信的主雷达、从雷达以及主控装置,主雷达和从雷达分别分布在铁路两侧,且两者之间的连线与铁路中心线垂直;In one embodiment, a catenary measurement system is provided, the catenary measurement system includes a master radar, a slave radar and a master control device that communicate with each other, the master radar and the slave radar are respectively distributed on both sides of the railway, and both The connection between them is perpendicular to the railway centerline;

主控装置根据预设的同步方案发送工作指令至主雷达和从雷达;The master control device sends work orders to the master radar and the slave radar according to the preset synchronization scheme;

主雷达和从雷达根据所述工作指令向接触网的同一测量点发射测量信号,且将接收到的雷达回波信号发送至主控装置;The main radar and the slave radar transmit measurement signals to the same measurement point of the catenary according to the work instruction, and send the received radar echo signals to the main control device;

主控装置分别根据主雷达及从雷达发送的初始观测时刻的雷达回波信号进行脉冲压缩得到相应的脉冲压缩图像,且分别识别出接触网在各脉冲压缩图像中的波峰位置以及获取所述波峰位置对应的波峰复数散射数据;The main control device performs pulse compression according to the main radar and the radar echo signal at the initial observation time sent from the radar to obtain corresponding pulse compression images, and respectively identifies the peak positions of the catenary in each pulse compression image and obtains the wave peaks. The peak complex scattering data corresponding to the position;

从预设的局部坐标系中提取主雷达和从雷达的实际坐标,根据各实际坐标以及相应的波峰复数散射数据进行计算,得到初始观测时刻所述接触网分别与主雷达和从雷达之间的初始距离,以及接触网的初始坐标;The actual coordinates of the master radar and the slave radar are extracted from the preset local coordinate system, and the calculation is performed according to the actual coordinates and the corresponding wave peak complex scattering data to obtain the relationship between the catenary and the master radar and the slave radar at the initial observation time. The initial distance, and the initial coordinates of the catenary;

根据多个观测时刻的雷达回波数据分别得到对应主雷达和从雷达的两组复散射观测向量,并根据两组复散射观测向量采用时间差分干涉方法得到每一观测时刻接触网分别相对于主雷达和从雷达之间的位移量;According to the radar echo data of multiple observation times, two sets of complex scattering observation vectors corresponding to the main radar and the secondary radar are obtained respectively, and according to the two sets of complex scattering observation vectors, the time difference interference method is used to obtain the relative relationship between the catenary and the main radar at each observation time. amount of displacement between the radar and the slave radar;

根据主雷达、从雷达的实际坐标、接触网的初始坐标、接触网分别与主雷达和从雷达之间的初始距离、以及每一观测时刻接触网分别相对于主雷达和从雷达之间的位移量,基于两点间求距离公式构建接触网的导高变化量及拉出值变化量为未知数的方程,并进行求解得到导高变化量以及拉出值变化量;According to the actual coordinates of the main radar and the subordinate radar, the initial coordinates of the catenary, the initial distance between the catenary and the main radar and the subordinate radar, and the displacement of the catenary relative to the main radar and the subordinate radar at each observation moment based on the formula for finding the distance between two points, construct the equations in which the change of lead height and the change of pull-out value of the catenary are unknowns, and solve it to obtain the change of lead-to-height and the change of pull-out value;

根据导高变化量以及拉出值变化量进行频谱分析得到接触网的力学参数。The mechanical parameters of the catenary are obtained by spectrum analysis according to the variation of the lead height and the variation of the pull-out value.

在其中一实施例中,主控装置在根据导高变化量以及拉出值变化量进行频谱分析得到所述接触网的力学参数之后还包括:In one of the embodiments, the main control device further includes: after performing spectrum analysis according to the variation of the lead height and the variation of the pull-out value to obtain the mechanical parameters of the catenary:

根据力学参数对接触网进行判断:The catenary is judged according to the mechanical parameters:

若力学参数符合预设的设计范围,则判断与观测时刻对应部分的接触网工作正常;If the mechanical parameters conform to the preset design range, it is judged that the catenary of the part corresponding to the observation time is working normally;

若力学参数不符合预设的设计范围,则判断该部分接触网存在潜在的故障。If the mechanical parameters do not meet the preset design range, it is judged that this part of the catenary has potential failures.

本领域普通技术人员可以理解实现上述实施例方法中的全部或部分流程,是可以通过计算机程序来指令相关的硬件来完成,所述的计算机程序可存储于一非易失性计算机可读取存储介质中,该计算机程序在执行时,可包括如上述各方法的实施例的流程。其中,本申请所提供的各实施例中所使用的对存储器、存储、数据库或其它介质的任何引用,均可包括非易失性和/或易失性存储器。非易失性存储器可包括只读存储器(ROM)、可编程ROM(PROM)、电可编程ROM(EPROM)、电可擦除可编程ROM(EEPROM)或闪存。易失性存储器可包括随机存取存储器(RAM)或者外部高速缓冲存储器。作为说明而非局限,RAM以多种形式可得,诸如静态RAM(SRAM)、动态RAM(DRAM)、同步DRAM(SDRAM)、双数据率SDRAM(DDRSDRAM)、增强型SDRAM(ESDRAM)、同步链路(Synchlink) DRAM(SLDRAM)、存储器总线(Rambus)直接RAM(RDRAM)、直接存储器总线动态RAM(DRDRAM)、以及存储器总线动态RAM(RDRAM)等。Those of ordinary skill in the art can understand that all or part of the processes in the methods of the above embodiments can be implemented by instructing relevant hardware through a computer program, and the computer program can be stored in a non-volatile computer-readable storage In the medium, when the computer program is executed, it may include the processes of the above-mentioned method embodiments. Wherein, any reference to memory, storage, database or other medium used in the various embodiments provided in this application may include non-volatile and/or volatile memory. Nonvolatile memory may include read only memory (ROM), programmable ROM (PROM), electrically programmable ROM (EPROM), electrically erasable programmable ROM (EEPROM), or flash memory. Volatile memory may include random access memory (RAM) or external cache memory. By way of illustration and not limitation, RAM is available in various forms such as static RAM (SRAM), dynamic RAM (DRAM), synchronous DRAM (SDRAM), double data rate SDRAM (DDRSDRAM), enhanced SDRAM (ESDRAM), synchronous chain Road (Synchlink) DRAM (SLDRAM), memory bus (Rambus) direct RAM (RDRAM), direct memory bus dynamic RAM (DRDRAM), and memory bus dynamic RAM (RDRAM) and so on.

以上实施例的各技术特征可以进行任意的组合,为使描述简洁,未对上述实施例中的各个技术特征所有可能的组合都进行描述,然而,只要这些技术特征的组合不存在矛盾,都应当认为是本说明书记载的范围。The technical features of the above embodiments can be combined arbitrarily. In order to make the description simple, all possible combinations of the technical features in the above embodiments are not described. However, as long as there is no contradiction in the combination of these technical features It is considered to be the range described in this specification.

以上所述实施例仅表达了本申请的几种实施方式,其描述较为具体和详细,但并不能因此而理解为对发明专利范围的限制。应当指出的是,对于本领域的普通技术人员来说,在不脱离本申请构思的前提下,还可以做出若干变形和改进,这些都属于本申请的保护范围。因此,本申请专利的保护范围应以所附权利要求为准。The above-mentioned embodiments only represent several embodiments of the present application, and the descriptions thereof are specific and detailed, but should not be construed as a limitation on the scope of the invention patent. It should be pointed out that for those skilled in the art, without departing from the concept of the present application, several modifications and improvements can be made, which all belong to the protection scope of the present application. Therefore, the scope of protection of the patent of the present application shall be subject to the appended claims.

Claims (9)

1. The method is characterized by being applied to a contact network measuring system, wherein the contact network measuring system comprises a main radar, a secondary radar and a main control device which are communicated with each other, the main radar and the secondary radar are respectively distributed on two sides of a railway, and a connecting line between the main radar and the secondary radar is perpendicular to a central line of the railway;
the railway contact network measuring method comprises the following steps:
the master control device sends a working instruction to the master radar and the slave radar according to a preset synchronization scheme;
the master radar and the slave radar transmit measurement signals to the same measurement point of the overhead line system according to the working instruction, and transmit the received radar echo signals to the master control device, or respectively perform pulse compression on the received radar echo signals to obtain compressed radar echo signals, and then transmit the compressed radar echo signals to the master control device;
the main control device respectively performs pulse compression according to radar echo signals at the initial observation time sent by a main radar and a slave radar to obtain corresponding pulse compression images, or the main control device directly converts the compressed radar echo signals received from the main radar and the slave radar into pulse compression images, respectively identifies the peak positions of the contact network in each pulse compression image, and acquires peak complex scattering data corresponding to the peak positions;
extracting actual coordinates of the main radar and the slave radar from a preset local coordinate system, and calculating according to each actual coordinate and corresponding peak complex scattering data to obtain an initial distance between the catenary and the main radar and the slave radar respectively at an initial observation moment and initial coordinates of the catenary;
respectively obtaining two groups of complex scattering observation vectors corresponding to the main radar and the slave radar according to radar echo data of a plurality of observation moments, and obtaining displacement of the overhead line system relative to the main radar and the slave radar at each observation moment by adopting a time difference interference method according to the two groups of complex scattering observation vectors;
according to the actual coordinates of the main radar, the actual coordinates of the auxiliary radar, the initial coordinates of the overhead line system, the initial distance between the overhead line system and the main radar and the initial distance between the overhead line system and the auxiliary radar respectively, and the displacement of the overhead line system relative to the main radar and the auxiliary radar at each observation moment, an equation with the overhead line system height variation and the pull-out value variation as unknowns is constructed based on a distance solving formula between two points, and the overhead line system height variation and the pull-out value variation are solved;
and carrying out spectrum analysis according to the lead height variation and the pull-out value variation to obtain the mechanical parameters of the overhead line system.
2. The radar system based railway catenary measurement method according to claim 1, wherein the preset synchronization scheme comprises a first synchronization scheme and a second synchronization scheme;
the first synchronization scheme comprises controlling the main radar and the auxiliary radar to transmit measurement signals with different frequencies or different codes at the same moment;
the second synchronization scheme includes controlling the master radar and the slave radar to alternately transmit measurement signals having the same frequency and the same code.
3. The method for measuring the railway contact network based on the radar system as claimed in claim 1, wherein the bandwidth of the measurement signals transmitted by the main radar and the secondary radar is more than 500 MHz.
4. The method for measuring the railway catenary based on the radar system as claimed in claim 1, wherein the method comprises the steps of extracting actual coordinates of the main radar and the secondary radar from a preset local coordinate system, calculating according to each actual coordinate and corresponding peak complex scattering data, and obtaining an initial distance between the catenary and the main radar and the secondary radar respectively at an initial observation time and an initial coordinate of the catenary, wherein after obtaining the initial distance between the catenary and the main radar and the secondary radar respectively at the initial observation time, the method comprises the following steps:
constructing a first equation with the initial coordinate of the overhead line system as an unknown number according to the actual coordinate of the main radar and the initial distance between the main radar and the overhead line system;
constructing a second equation with the initial coordinate of the overhead line system as an unknown number according to the actual coordinate of the slave radar and the initial distance between the slave radar and the overhead line system;
and solving by using a first equation and a second equation to obtain the initial coordinate of the overhead line system.
5. The method for measuring the railway overhead line system based on the radar system as claimed in claim 1, wherein the step of constructing an equation with the overhead line system variation and the pull-out value variation as unknowns based on a distance solving formula between two points according to the actual coordinates of the main radar and the slave radar, the initial coordinates of the overhead line system, the initial distances between the overhead line system and the main radar and the slave radar respectively, and the displacement of the overhead line system relative to the main radar and the slave radar at each observation moment, and solving to obtain the overhead line variation and the pull-out value variation comprises the steps of:
setting the initial observation time as the previous observation time;
constructing a first distance equation between the main radar and the overhead contact system at the current observation time according to the actual coordinates of the main radar, the initial coordinates of the overhead contact system, the variation of the guide height, the variation of the pull-out value, the initial distance between the main radar and the overhead contact system and the displacement of the overhead contact system relative to the main radar at the current observation time;
constructing a second distance equation between the slave radar and the overhead contact system at the current observation time according to the actual coordinates of the slave radar, the initial coordinates of the overhead contact system, the variation of the guide height, the variation of the pull-out value, the initial distance between the slave radar and the overhead contact system and the displacement of the overhead contact system relative to the slave radar at the current observation time;
and solving the first distance equation and the second distance equation at a plurality of observation moments respectively to obtain the derivative variation and the pull-out value variation corresponding to each observation moment.
6. The method for measuring the railway overhead line system based on the radar system of claim 5, wherein the obtaining of the mechanical parameters of the overhead line system by performing spectrum analysis according to the variation of the overhead line system and the variation of the pull-out value comprises:
respectively finding out the maximum lead height change amount and the maximum pull-out value change amount from the lead height change amount and the pull-out value change amount corresponding to each observation moment, and respectively calculating and correspondingly obtaining a lead height impact amplitude and a pull-out value impact amplitude according to the maximum lead height change amount and the maximum pull-out value change amount;
and carrying out Fourier transform according to the lead height variation corresponding to each observation time to obtain a lead height variation frequency spectrum, extracting a fundamental frequency component from the lead height variation frequency spectrum, and estimating the tension of the contact network cable, the linear density of the chord cable and the equivalent length of the contact network cable according to the fundamental frequency component and a tension formula of the contact network cable to obtain a tension estimated value, a linear density estimated value and an equivalent length estimated value.
7. The method for measuring the railway overhead line system based on the radar system according to any one of claims 1 to 6, wherein the method for measuring the railway overhead line system further comprises the following steps of after obtaining mechanical parameters of the overhead line system through spectrum analysis according to the variation of the overhead line system and the variation of the pull-out value:
judging the contact network according to the mechanical parameters:
if the mechanical parameters accord with a preset design range, judging that the part of the contact net corresponding to the observation moment works normally;
and if the mechanical parameters do not accord with the preset design range, judging that the part of the contact network has potential faults.
8. The contact network measuring system based on the radar system is characterized by comprising a main radar, a secondary radar and a main control device which are communicated with each other, wherein the main radar and the secondary radar are respectively distributed on two sides of a railway, and a connecting line between the main radar and the secondary radar is vertical to the central line of the railway;
the master control device sends a working instruction to the master radar and the slave radar according to a preset synchronization scheme;
the master radar and the slave radar transmit measurement signals to the same measurement point of the overhead line system according to the working instruction, and transmit the received radar echo signals to the master control device;
the main control device respectively performs pulse compression according to radar echo signals at the initial observation time sent by a main radar and a slave radar to obtain corresponding pulse compression images, respectively identifies the peak position of the contact network in each pulse compression image and acquires peak complex scattering data corresponding to the peak position;
extracting actual coordinates of the main radar and the slave radar from a preset local coordinate system, and calculating according to each actual coordinate and corresponding peak complex scattering data to obtain initial distances between the catenary and the main radar and the slave radar respectively at an initial observation moment and initial coordinates of the catenary;
respectively obtaining two groups of complex scattering observation vectors corresponding to the main radar and the slave radar according to radar echo data of a plurality of observation moments, and obtaining displacement of the overhead line system relative to the main radar and the slave radar at each observation moment by adopting a time difference interference method according to the two groups of complex scattering observation vectors;
according to the actual coordinates of the main radar, the actual coordinates of the auxiliary radar, the initial coordinates of the overhead line system, the initial distance between the overhead line system and the main radar and the initial distance between the overhead line system and the auxiliary radar respectively, and the displacement of the overhead line system relative to the main radar and the auxiliary radar at each observation moment, an equation with the overhead line system height variation and the pull-out value variation as unknowns is constructed based on a distance solving formula between two points, and the overhead line system height variation and the pull-out value variation are solved;
and carrying out spectrum analysis according to the lead height variation and the pull-out value variation to obtain the mechanical parameters of the overhead line system.
9. The catenary measurement system according to claim 8, wherein the main control device, after performing spectrum analysis according to the lead height variation and the pull-out value variation to obtain the mechanical parameters of the catenary, further comprises:
judging the contact network according to the mechanical parameters:
if the mechanical parameters accord with a preset design range, judging that the part of the contact net corresponding to the observation moment works normally;
and if the mechanical parameters do not accord with the preset design range, judging that the part of the contact network has potential faults.
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