CN115993485A - Estimation Method of Equivalent Relative Permittivity of Parallel Pair Multi-Core Cables - Google Patents
Estimation Method of Equivalent Relative Permittivity of Parallel Pair Multi-Core Cables Download PDFInfo
- Publication number
- CN115993485A CN115993485A CN202211613576.6A CN202211613576A CN115993485A CN 115993485 A CN115993485 A CN 115993485A CN 202211613576 A CN202211613576 A CN 202211613576A CN 115993485 A CN115993485 A CN 115993485A
- Authority
- CN
- China
- Prior art keywords
- dielectric constant
- cable
- crosstalk
- relative dielectric
- equivalent relative
- 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.)
- Pending
Links
- 238000000034 method Methods 0.000 title claims abstract description 32
- 238000001228 spectrum Methods 0.000 claims abstract description 38
- 230000005540 biological transmission Effects 0.000 claims description 17
- 239000004020 conductor Substances 0.000 claims description 9
- 238000009413 insulation Methods 0.000 claims description 5
- 238000001514 detection method Methods 0.000 abstract description 5
- 238000005259 measurement Methods 0.000 abstract description 4
- 239000011810 insulating material Substances 0.000 abstract description 2
- 238000004519 manufacturing process Methods 0.000 abstract 1
- 230000000737 periodic effect Effects 0.000 description 6
- 238000010586 diagram Methods 0.000 description 5
- 239000000463 material Substances 0.000 description 5
- 239000011159 matrix material Substances 0.000 description 5
- 230000015556 catabolic process Effects 0.000 description 3
- 238000006731 degradation reaction Methods 0.000 description 3
- 230000001066 destructive effect Effects 0.000 description 3
- 229920000295 expanded polytetrafluoroethylene Polymers 0.000 description 3
- 239000012774 insulation material Substances 0.000 description 3
- 238000012545 processing Methods 0.000 description 3
- 239000003990 capacitor Substances 0.000 description 2
- 230000001419 dependent effect Effects 0.000 description 2
- 239000006185 dispersion Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000005070 sampling Methods 0.000 description 2
- 101001121408 Homo sapiens L-amino-acid oxidase Proteins 0.000 description 1
- 101000827703 Homo sapiens Polyphosphoinositide phosphatase Proteins 0.000 description 1
- 102100026388 L-amino-acid oxidase Human genes 0.000 description 1
- 102100023591 Polyphosphoinositide phosphatase Human genes 0.000 description 1
- 101100233916 Saccharomyces cerevisiae (strain ATCC 204508 / S288c) KAR5 gene Proteins 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 238000004364 calculation method Methods 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 230000002427 irreversible effect Effects 0.000 description 1
- 238000012417 linear regression Methods 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000035939 shock Effects 0.000 description 1
- 238000012360 testing method Methods 0.000 description 1
- 238000012795 verification Methods 0.000 description 1
Images
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E60/00—Enabling technologies; Technologies with a potential or indirect contribution to GHG emissions mitigation
Landscapes
- Measurement Of Resistance Or Impedance (AREA)
Abstract
Description
技术领域Technical Field
本发明涉及一种平行对多芯电缆等效相对介电常数估计方法,属于电缆参数测量技术领域。The invention relates to a method for estimating the equivalent relative dielectric constant of a parallel multi-core cable, belonging to the technical field of cable parameter measurement.
背景技术Background Art
高速数据电缆的等效相对介电常数是一项重要参数,直接决定了电缆中的波速的大小和时延情况。除此之外,等效相对介电常数对电缆质量一致性和性能退化的估计中也有重要作用。一方面,新生产电缆的等效相对介电常数主要受到电缆材料的品质和加工过程中工艺步骤的影响,因此等效相对介电常数可以作为不同批次电缆之间质量一致性的判断依据;另一方面,电缆在使用过程中受到机械冲击、过高温升等因素的影响,其机械结构和材料性能均可能发生改变,导致其包括等效相对介电常数在内的性能参数发生退化,因此等效相对介电常数也可以作为表征服役中电缆性能退化情况的重要参数。传统的低频介电常数测算方法为平板电容法,需要将待测材料制作成圆柱状样品,插入平行极板构成的夹具中,通过测量构成的电容器的电容来计算相对介电常数;高频可以采用传输线法,也需要将柱状样品插入到同轴型夹具中,通过测量插入样品后的散射参数来计算相对介电常数。将这些方法用于电缆绝缘材料介电常数的检测时,需要将待测材料制作成特定形状的样品,不仅会对待测电缆造成不可逆破坏,使其不可能再正常工作,而且加工样品的过程也可能影响到材料的介电参数,使测试值偏离实际值。因此,最理想的电缆绝缘介电常数测量方法应该是利用电缆的结构特点,通过合适的传输特性对其介电常数进行测算。基于同轴电缆的结构特点,IEC 61196-1-125标准阐述了利用电缆两端的相位差计算其等效相对介电常数的方法,但此方法不适用于均匀性较差的非同轴电缆。The equivalent relative dielectric constant of high-speed data cables is an important parameter that directly determines the size of the wave velocity and time delay in the cable. In addition, the equivalent relative dielectric constant also plays an important role in estimating the quality consistency and performance degradation of cables. On the one hand, the equivalent relative dielectric constant of newly produced cables is mainly affected by the quality of cable materials and the process steps in the processing process. Therefore, the equivalent relative dielectric constant can be used as a basis for judging the quality consistency between different batches of cables; on the other hand, the cable may be affected by mechanical shock, excessive temperature rise and other factors during use, and its mechanical structure and material properties may change, resulting in the degradation of its performance parameters including the equivalent relative dielectric constant. Therefore, the equivalent relative dielectric constant can also be used as an important parameter to characterize the performance degradation of cables in service. The traditional low-frequency dielectric constant measurement method is the flat plate capacitor method, which requires the material to be tested to be made into a cylindrical sample, inserted into a fixture composed of parallel plates, and the relative dielectric constant is calculated by measuring the capacitance of the capacitor; the high frequency can use the transmission line method, which also requires the cylindrical sample to be inserted into a coaxial fixture, and the relative dielectric constant is calculated by measuring the scattering parameters after the sample is inserted. When these methods are used to detect the dielectric constant of cable insulation materials, the material to be tested needs to be made into a sample of a specific shape, which will not only cause irreversible damage to the cable to be tested, making it impossible for it to work normally, but also the process of processing the sample may affect the dielectric parameters of the material, causing the test value to deviate from the actual value. Therefore, the most ideal method for measuring the dielectric constant of cable insulation should be to use the structural characteristics of the cable and calculate its dielectric constant through appropriate transmission characteristics. Based on the structural characteristics of coaxial cables, the IEC 61196-1-125 standard describes a method for calculating its equivalent relative dielectric constant using the phase difference between the two ends of the cable, but this method is not suitable for non-coaxial cables with poor uniformity.
发明内容Summary of the invention
针对如何实现对电缆等效介电常数的非侵入式快速无损检测的问题,本发明提供一种平行对多芯电缆等效相对介电常数估计方法。In order to solve the problem of how to realize non-invasive rapid non-destructive detection of equivalent dielectric constant of cables, the present invention provides a method for estimating equivalent relative dielectric constant of multi-core cables in parallel.
本发明的一种平行对多芯电缆等效相对介电常数估计方法,包括:A method for estimating the equivalent relative dielectric constant of a multi-core cable in parallel of the present invention comprises:
步骤1、制作长度为l的电缆样品;Step 1, making a cable sample with a length of l;
步骤2、利用矢量网络分析仪测量电缆样品的串扰频谱;Step 2: Use a vector network analyzer to measure the crosstalk spectrum of the cable sample;
步骤3、辨识出串扰频谱中的极大值点或极小值点,计算极大值点或极小值点之间的平均频率差Δf,根据平均频率差获得电缆样品的等效相对介电常数的估计值 Step 3: Identify the maximum or minimum points in the crosstalk spectrum, calculate the average frequency difference Δf between the maximum or minimum points, and obtain an estimated value of the equivalent relative dielectric constant of the cable sample based on the average frequency difference.
c表示真空中的光速。c is the speed of light in vacuum.
作为优选,步骤3中,平均频率差为:Preferably, in
将辨识出的s个极大值点或极小值点由小到大排列成频率点序列fi,i=1,2,…,s,s表示极大值点或极小值点的数量; Arrange the identified s maximum or minimum points from small to large into a frequency point sequence fi , i = 1, 2, ..., s, s represents the number of maximum or minimum points;
作为优选,步骤3中,辨识出串扰频谱中的极大值点nmax或极小值点nmin满足:Preferably, in
A(nmax)≥max{A(nmax-t:nmax+t)}A(n max )≥max{A(n max -t:n max +t)}
A(nmin)≤min{A(nmin-t:nmin+t)}A(n min )≤min{A(n min -t:n min +t)}
其中,A(n1:n2)表示第n1到第n2个频率点的串扰幅值构成的集合,t表示极值点搜索范围阈值,A(nmax)表示极大值点nmax的串扰幅值,A(nmin)表示极小值点nmin的串扰幅值。Wherein, A(n 1 :n 2 ) represents the set of crosstalk amplitudes from the n 1th to the n 2th frequency points, t represents the extreme point search range threshold, A(n max ) represents the crosstalk amplitude of the maximum point n max , and A(n min ) represents the crosstalk amplitude of the minimum point n min .
作为优选,步骤3中,极值点搜索范围阈值t满足:Preferably, in
N表示矢量网络分析仪采样的总频率点数,fM表示待估计频率范围上限,fm表示待估计频率范围下限,εrM表示等效介电常数上限值。N represents the total number of frequency points sampled by the vector network analyzer, fM represents the upper limit of the frequency range to be estimated, fm represents the lower limit of the frequency range to be estimated, and εrM represents the upper limit of the equivalent dielectric constant.
作为优选,步骤3中,若按照极值点搜索范围阈值t辨识出串扰频谱中的极大值点或极小值点的数量s与期望不符,则增加矢量网络分析仪采样的总频率点数N。Preferably, in
作为优选,步骤1中,长度l:Preferably, in step 1, the length l is:
fm表示待估计频率范围下限,εrM表示等效介电常数上限值,εrm表示等效介电常数下限值。f m represents the lower limit of the frequency range to be estimated, ε rM represents the upper limit of the equivalent dielectric constant, and ε rm represents the lower limit of the equivalent dielectric constant.
本发明的有益效果,本发明在一定频率范围内对其平均等效相对介电常数进行测量的方法,通过测量屏蔽平行对电缆芯线之间的串扰幅值频谱来计算其相对介电常数,无需破坏电缆结构以制作电缆绝缘材料的样品,可以实现对电缆等效介电常数的非侵入式快速无损检测。The beneficial effects of the present invention are as follows: the method for measuring the average equivalent relative dielectric constant within a certain frequency range of the present invention calculates the relative dielectric constant by measuring the crosstalk amplitude spectrum between the shielded parallel cable cores, and there is no need to destroy the cable structure to prepare samples of the cable insulation material, thereby realizing non-invasive, rapid and non-destructive detection of the equivalent dielectric constant of the cable.
附图说明BRIEF DESCRIPTION OF THE DRAWINGS
图1为本发明测量电路原理图;FIG1 is a schematic diagram of a measuring circuit of the present invention;
图2为连接矢网与电缆间的连接件样例;Figure 2 is an example of a connector between a vector network and a cable;
图3为串扰频谱中的局部扰动示意图,横坐标为频率,纵坐标为串扰振幅;FIG3 is a schematic diagram of a local disturbance in a crosstalk spectrum, where the abscissa is the frequency and the ordinate is the crosstalk amplitude;
图4为25℃时测得的串扰频谱图和辨识出的极大值点分布图,横坐标为频率,纵坐标为串扰振幅;FIG4 is a crosstalk spectrum diagram measured at 25°C and a distribution diagram of the identified maximum points, where the horizontal axis is the frequency and the vertical axis is the crosstalk amplitude;
图5为不同温度下测算得到的等效相对介电常数散点图,横坐标为温度,纵坐标为等效相对介电常数。FIG5 is a scatter plot of the equivalent relative dielectric constant calculated at different temperatures, where the abscissa is temperature and the ordinate is the equivalent relative dielectric constant.
具体实施方式DETAILED DESCRIPTION
下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有作出创造性劳动的前提下所获得的所有其他实施例,都属于本发明保护的范围。The following will be combined with the drawings in the embodiments of the present invention to clearly and completely describe the technical solutions in the embodiments of the present invention. Obviously, the described embodiments are only part of the embodiments of the present invention, not all of the embodiments. Based on the embodiments of the present invention, all other embodiments obtained by ordinary technicians in this field without creative work are within the scope of protection of the present invention.
需要说明的是,在不冲突的情况下,本发明中的实施例及实施例中的特征可以相互组合。It should be noted that, in the absence of conflict, the embodiments of the present invention and the features in the embodiments may be combined with each other.
下面结合附图和具体实施例对本发明作进一步说明,但不作为本发明的限定。The present invention will be further described below in conjunction with the accompanying drawings and specific embodiments, but they are not intended to limit the present invention.
本实施方式基于串扰频谱来计算平行对电缆的等效相对介电常数:一定长度的含屏蔽层的平行对电缆可以视为一个典型的三导体传输线系统,其串扰幅值受到频率的影响。当电缆传输高频电磁波时,电缆为电气长线,电缆上的波过程不能忽略,串扰受扰线的近端串扰信号受到电缆上波的叠加作用影响,呈现近似随频率周期性变化的关系,表现为串扰幅值随频率的周期性变化,变化的频率周期与电缆上电磁波的波长暨等效相对介电常数直接相关。受到电缆衰减、布置方式的影响,串扰幅值的频谱并非完美的周期性谱线,可以通过一定频率范围串扰频谱的极大值点或极小值点之间的平均间隔估计串扰频谱的频率周期,进而估算一定频率范围内电缆的平均等效相对介电常数。This implementation method calculates the equivalent relative dielectric constant of parallel cables based on the crosstalk spectrum: a certain length of parallel cables with a shielding layer can be regarded as a typical three-conductor transmission line system, and its crosstalk amplitude is affected by the frequency. When the cable transmits high-frequency electromagnetic waves, the cable is an electrical long line, and the wave process on the cable cannot be ignored. The near-end crosstalk signal of the crosstalk-affected line is affected by the superposition of the waves on the cable, showing an approximate periodic change with the frequency, which is manifested as a periodic change of the crosstalk amplitude with the frequency. The frequency period of the change is directly related to the wavelength of the electromagnetic wave on the cable and the equivalent relative dielectric constant. Affected by the attenuation and layout of the cable, the spectrum of the crosstalk amplitude is not a perfect periodic spectrum line. The frequency period of the crosstalk spectrum can be estimated by the average interval between the maximum or minimum points of the crosstalk spectrum in a certain frequency range, and then the average equivalent relative dielectric constant of the cable in a certain frequency range can be estimated.
关于忽略色散效应、无损条件下的三导体近端串扰频谱幅值随频率的周期性变化的证明:Proof of the periodic variation of the amplitude of the three-conductor near-end crosstalk spectrum with frequency under lossless conditions, ignoring the dispersion effect:
考虑无损的均匀三导体传输线问题,定义:Consider a lossless uniform three-conductor transmission line problem and define:
L、C分别表示传输线电流向量、传输线电压向量、传输线单位长度电感参数矩阵、传输线单位长度电容参数矩阵;分别表示串扰发射线和串扰接收线上位置z处的电流相量;分别表示串扰发射线和串扰接收线上位置z处的电压相量;lG、lm、lR分别表示串扰发射线的自电感、串扰接收线的自电感、串扰发射线与串扰接收线之间的互电感;cG、cm、cR分别表示串扰发射线的自电容、串扰接收线的自电容、串扰发射线与串扰接收线之间的互电容; L and C represent the transmission line current vector, the transmission line voltage vector, the transmission line unit length inductance parameter matrix, and the transmission line unit length capacitance parameter matrix respectively; represent the current phasors at position z on the crosstalk transmitting line and the crosstalk receiving line respectively; Respectively represent the voltage phasors at position z on the crosstalk transmitting line and the crosstalk receiving line; l G , l m , l R represent the self-inductance of the crosstalk transmitting line, the self-inductance of the crosstalk receiving line, and the mutual inductance between the crosstalk transmitting line and the crosstalk receiving line; c G , cm , c R represent the self-capacitance of the crosstalk transmitting line, the self-capacitance of the crosstalk receiving line, and the mutual capacitance between the crosstalk transmitting line and the crosstalk receiving line;
则有频域的无损三导体传输线方程:Then there is a lossless three-conductor transmission line equation in the frequency domain:
又定义终端源和阻抗矩阵:The terminal source and impedance matrix are defined as follows:
VS、RS、RL分别表示源端电压向量、源端电阻向量、负载端电阻向量;RS、RNE、RL、RFE分别表示串扰发射线源端电压、串扰发射线源端输出电阻、串扰接收线源端输出电阻、串扰发射线负载端输入电阻、串扰接收线负载端输入电阻。V S , R S , and RL represent the source terminal voltage vector, source terminal resistance vector, and load terminal resistance vector, respectively; R S , R NE , R L , and R FE represent the voltage at the source end of the crosstalk transmission line, the output resistance at the source end of the crosstalk transmission line, the output resistance at the source end of the crosstalk receiving line, the input resistance at the load end of the crosstalk transmission line, and the input resistance at the load end of the crosstalk receiving line, respectively.
则长度为L的传输线的解满足终端条件:Then the solution for a transmission line of length L satisfies the terminal condition:
此时的传输线方程是解耦的,由(5)(6)可解得链参数矩阵:The transmission line equation is decoupled at this time, and the chain parameter matrix can be solved by (5) (6):
其中:in:
Φ11=cos(βL)12 (13)Φ 11 =cos(βL)1 2 (13)
Φ22=cos(βL)12 (16)Φ 22 = cos(βL)1 2 (16)
β表示三导体传输线系统的传播常数,12表示二阶单位矩阵。β represents the propagation constant of the three-conductor transmission line system, and 1 2 represents the second-order unit matrix.
结合终端条件(10)(11)可得:Combining the terminal conditions (10) and (11) we can obtain:
对于(17),取负载两条导线与地之间的电阻相等,均为R,则(17)变为:For (17), the resistance between the two load wires and the ground is equal, both R, then (17) becomes:
两侧同除以R,得到:Dividing both sides by R, we get:
令R趋于正无穷,等效于两线的负载端开路的情况,以上方程变为:Let R tend to positive infinity, which is equivalent to the case where the load ends of the two wires are open circuited, and the above equation becomes:
展开为:Expands to:
考虑到波速利用Cramer法则,容易求出串扰接收端电流:Considering the wave speed Using Cramer's law, it is easy to find the crosstalk receiving end current:
B=cmcos(βL)+jvsin(βL)(cG+cm)cm(RS-RNE) (25)B=c m cos(βL)+jvsin(βL)(c G +c m )c m ( RS -R NE ) (25)
记为电缆的电角度,则:remember is the electrical angle of the cable, then:
忽略色散效应,VR(0)是关于θ的以π为周期的周期函数,也即关于L的以λ/2为周期的函数,关于频率的以为周期的函数。Ignoring the dispersion effect, VR (0) is a periodic function with a period of π about θ, which is also a periodic function with a period of λ/2 about L. of is a function of the period.
本实施方式的平行对多芯电缆等效相对介电常数估计方法,包括:The method for estimating the equivalent relative dielectric constant of a multi-core cable in parallel of this embodiment includes:
步骤1、根据所需估计频带,确定电缆样品的长度l,制作电缆样品;Step 1: Determine the length l of the cable sample according to the required estimated frequency band, and make the cable sample;
步骤2、利用矢量网络分析仪测量电缆样品的串扰频谱;Step 2: Use a vector network analyzer to measure the crosstalk spectrum of the cable sample;
步骤3、辨识出串扰频谱中的极大值点或极小值点,计算极大值点或极小值点之间的平均频率差Δf,根据平均频率差获得电缆样品的等效相对介电常数的估计值 Step 3: Identify the maximum or minimum points in the crosstalk spectrum, calculate the average frequency difference Δf between the maximum or minimum points, and obtain an estimated value of the equivalent relative dielectric constant of the cable sample based on the average frequency difference.
本实施方式中,根据串扰频谱幅值随频率的周期性变化的结论,从变化的频率周期与电缆上电磁波的波长也即等效相对介电常数直接相关,可以确定串扰频谱极值点间的平均频率差满足以下关系:In this implementation, based on the conclusion that the amplitude of the crosstalk spectrum changes periodically with frequency, the changing frequency period is directly related to the wavelength of the electromagnetic wave on the cable, that is, the equivalent relative dielectric constant. It can be determined that the average frequency difference between the extreme points of the crosstalk spectrum satisfies the following relationship:
易得:Easy to get:
c表示真空中的光速。c is the speed of light in vacuum.
本实施方式通过测量屏蔽平行对电缆芯线之间的串扰幅值频谱来计算其相对介电常数,无需破坏电缆结构以制作电缆绝缘材料的样品,可以实现对电缆等效介电常数的非侵入式快速无损检测。This embodiment calculates the relative dielectric constant of a shielded parallel pair of cables by measuring the crosstalk amplitude spectrum between the core wires. There is no need to destroy the cable structure to make samples of the cable insulation material, and non-invasive, rapid and non-destructive detection of the equivalent dielectric constant of the cable can be achieved.
本实施方式的步骤1中制作平行对电缆样品,所用的平行对电缆需要包含屏蔽层,以形成三导体系统而产生串扰现象。假设待估计的频率范围[fm,fM],则一般fM<10fm,以保证相邻频谱极大值或极小值点间有均匀而充足的频率点数。电缆样品的长度由待估计频率范围下限fm确定,用以下公式估算:In step 1 of this embodiment, a parallel pair cable sample is prepared. The parallel pair cable used needs to include a shielding layer to form a three-conductor system to generate crosstalk. Assuming the frequency range to be estimated is [f m ,f M ], then generally f M <10f m to ensure that there are uniform and sufficient frequency points between adjacent spectrum maxima or minima. The length of the cable sample is determined by the lower limit of the frequency range to be estimated, f m , and is estimated using the following formula:
式中,l表示需制作的电缆样品的长度;c表示真空中的光速,约为3×108m/s;εrM表示等效介电常数上限值;εrm表示等效介电常数下限值。其中等效介电常数的上下限εrM和εrm可以由绝缘材料的类型或电缆的标称波速估计得到。In the formula, l represents the length of the cable sample to be manufactured; c represents the speed of light in a vacuum, which is approximately 3×10 8 m/s; ε rM represents the upper limit of the equivalent dielectric constant; and ε rm represents the lower limit of the equivalent dielectric constant. The upper and lower limits of the equivalent dielectric constant, ε rM and ε rm, can be estimated from the type of insulating material or the nominal wave velocity of the cable.
依据计算得到的电缆长度制作电缆样品,将其一端剖开约1cm分离出两根单芯电缆和屏蔽层,去除单芯电缆外适当长度的绝缘使导体露出,便于矢量网络分析仪端口连接。A cable sample was made based on the calculated cable length. One end was cut open by about 1 cm to separate the two single-core cables and the shielding layer. An appropriate length of insulation outside the single-core cable was removed to expose the conductor for easy connection to the vector network analyzer port.
本实施方式的步骤2中,串扰频谱测量时的电路图如图1所示。其中,电缆一端的两根芯线C、V经过连接件分别与矢量网络分析仪的两个端口Port 1和Port 2的信号线连接,绝缘层G经连接件与矢量网络分析仪的两个端口的地线连接,而电缆的另一端完全开路。In
连接件的作用完成矢量网络分析仪的同轴端口向电缆的屏蔽平行对端口的转换,同时起到减少电磁波的反射、增强串扰频谱测量结果的准确性的作用。连接件可以用PCB板制作,两端可以分别采用SMA座和接线座,传输线部分可以设计为尽可能短的50Ω微带线以与矢量网络分析仪匹配,如图2所示。The connector completes the conversion of the coaxial port of the vector network analyzer to the shielded parallel pair port of the cable, and at the same time reduces the reflection of electromagnetic waves and enhances the accuracy of the crosstalk spectrum measurement results. The connector can be made of PCB board, and the two ends can use SMA sockets and terminal sockets respectively. The transmission line part can be designed as a 50Ω microstrip line as short as possible to match the vector network analyzer, as shown in Figure 2.
完成电路的搭建后,即可利用矢量网络分析仪测量串扰频谱。配置矢量网络分析仪时,其频率上下限设为fM和fm,扫频点数应尽可能多,扫频方式设为线性扫描,信号功率选择可选范围内的最大功率。如果按照图1所示的方式连接,则矢量网络分析仪测得的S21即为串扰频谱。After the circuit is built, the crosstalk spectrum can be measured using a vector network analyzer. When configuring the vector network analyzer, set the upper and lower frequency limits to f M and f m , the number of sweep points should be as large as possible, the sweep mode should be set to linear sweep, and the signal power should be the maximum power within the optional range. If connected as shown in Figure 1, the S21 measured by the vector network analyzer is the crosstalk spectrum.
本实施方式的步骤3在测量得到矢量网络分析仪的S21数据暨近端串扰频谱之后,经过数据处理即可得到电缆的等效相对介电常数。首先辨识串扰出串扰频谱中的极大(或极小)值点,再计算这些极值点之间的平均频率差,以此估计一定频率范围内的波速进而计算等效介电常数。In
步骤31、辨识极值点:Step 31: Identify extreme points:
理想情况下,近端串扰频谱在待辨识的极值大值点与极小值点之间是单调的,考虑到矢量网络分析仪测量不同频率点的串扰数据以概率为1不相等,极大(小)值点满足的条件是此点的串扰幅值大于(小于)左右两点的串扰幅值,即:Ideally, the near-end crosstalk spectrum is monotonic between the extreme maximum value point and the minimum value point to be identified. Considering that the crosstalk data measured by the vector network analyzer at different frequency points are not equal with probability 1, the condition satisfied by the maximum (minimum) value point is that the crosstalk amplitude at this point is greater (less) than the crosstalk amplitudes of the left and right points, that is:
A(nmax-1)<A(nmax)>A(nmax+1) (32)A(n max -1)<A(n max )>A(n max +1) (32)
A(nmin-1)>A(nmin)<A(nmin+1) (33)A(n min -1)>A(n min )<A(n min +1) (33)
式中,A(n)表示第n个频率点的串扰幅值,n是离散扫频点由小到大的序号;nmax表示极大值点的序号;nmax表示极小值点的序号。Where A(n) represents the crosstalk amplitude at the nth frequency point, n is the number of discrete frequency sweep points from small to large, n max represents the number of the maximum point, and n max represents the number of the minimum point.
而实际上,受到电缆本身工艺水平导致的不均匀、连接点之间的反射、外界电磁干扰等因素的影响,串扰频谱可能存在微小的抖动,如图3圈中所示,导致满足式(32)或(33)的点不一定是期望辨识出的点。In fact, due to the unevenness of the cable's own process level, reflections between connection points, external electromagnetic interference and other factors, the crosstalk spectrum may have slight jitter, as shown in the circle in Figure 3, resulting in the point that satisfies equation (32) or (33) is not necessarily the point expected to be identified.
考虑到此类抖动点是附近很小范围内的局部最大(最小)值点,而期望辨识的极值点是附近,可以改进式(32)和式(33)方法,极值点满足:Considering that such jitter points are local maximum (minimum) value points in a small range nearby, and the extreme value points to be identified are nearby, the methods of equations (32) and (33) can be improved, and the extreme value points satisfy:
A(nmax)≥max{A(nmax-t:nmax+t)} (34)A(n max )≥max{A(n max -t:n max +t)} (34)
A(nmin)≤min{A(nmin-t:nmin+t)} (35)A(n min )≤min{A(n min -t:n min +t)} (35)
式中,A(n1:n2)表示第n1到第n2个频率点的串扰幅值构成的集合;t表示极值点搜索范围。Wherein, A(n 1 :n 2 ) represents the set of crosstalk amplitudes from the n 1th to the n 2th frequency points; t represents the extreme point search range.
搜索范围t的选取对极值点的成功辨识很重要:t选取过小时,无法有效剔除抖动点的干扰;t选取过大以至于大于部分相邻极值点间的频率间隔时,可能漏掉部分期望辨识出的极值点。这两种情况都会导致估计出的等效介电常数的错误,t可以按照以下公式选取:The selection of the search range t is very important for the successful identification of extreme points: if t is selected too small, the interference of jitter points cannot be effectively eliminated; if t is selected too large and larger than the frequency interval between some adjacent extreme points, some extreme points expected to be identified may be missed. Both of these situations will lead to errors in the estimated equivalent dielectric constant. t can be selected according to the following formula:
式中N表示矢量网络分析仪采样的总频率点数。Where N represents the total number of frequency points sampled by the vector network analyzer.
可以通过观察串扰频谱人工数出期望辨识的频率点数量,如果按照(36)选择的t辨识出的极值点个数与期望不符,说明矢量网络分析仪的总采样点数N不足,增加矢量网络分析仪采样的总频率点数N。The number of frequency points expected to be identified can be manually counted by observing the crosstalk spectrum. If the number of extreme points identified according to t selected by (36) does not match the expectation, it means that the total number of sampling points N of the vector network analyzer is insufficient, and the total number of frequency points N sampled by the vector network analyzer should be increased.
步骤32、计算等效相对介电常数:Step 32, calculate the equivalent relative dielectric constant:
将辨识出的s个极大值点或极小值点由小到大排列成频率点序列fi:Arrange the identified s maximum or minimum points from small to large into a frequency point sequence fi :
f1<f2<...<fs-1<fs (37)f 1 <f 2 <...<f s-1 <f s (37)
i=1,2,…,s,s表示极大值点或极小值点的数量;i=1,2,…,s, s represents the number of maximum or minimum points;
以下标i为自变量,频率点fi为因变量,考虑将其拟合为:The index i is the independent variable and the frequency point fi is the dependent variable. Consider fitting it as:
fi=ai+b (38) fi = ai + b (38)
这是一个典型的线性回归问题,利用最小二乘法拟合的结果为:This is a typical linear regression problem. The result of least squares fitting is:
其中:in:
显然,待求的平均频率差为:Obviously, the average frequency difference to be calculated is:
得到:get:
根据Δf,利用式(30)计算电缆样品的等效相对介电常数的估计值 According to Δf, the estimated value of the equivalent relative dielectric constant of the cable sample is calculated using formula (30):
实验验证:以一种ePTFE(膨体聚四氟乙烯)绝缘的平行对电缆为例,欲估计其在200MHz~1.2GHz范围内的平均等效相对介电常数。由生产厂家提供的参数资料得出其相对介电常数在区间[1.0,2.0]之中,按照(31)计算后选定样品的长度l=5m,所用矢量网络分析仪的最大采样点数为4001。Experimental verification: Taking an ePTFE (expanded polytetrafluoroethylene) insulated parallel pair cable as an example, we want to estimate its average equivalent relative dielectric constant in the range of 200MHz to 1.2GHz. The parameter data provided by the manufacturer show that its relative dielectric constant is in the interval [1.0, 2.0]. According to (31), the sample length l = 5m is selected after calculation, and the maximum number of sampling points of the vector network analyzer used is 4001.
将其置于恒温箱中,连接好串扰测量电路,分别测量了25~140℃的一些离散温度点条件下电缆近端串扰频谱。取t=20,25℃下的近端串扰频谱和辨识出的串扰极大值点位置如图4所示。It was placed in a constant temperature box, connected to the crosstalk measurement circuit, and the near-end crosstalk spectrum of the cable was measured at some discrete temperature points from 25 to 140°C. The near-end crosstalk spectrum at t=20, 25°C and the identified crosstalk maximum point position are shown in Figure 4.
采用相同的方法分析、计算出各温度下的等效相对介电常数,得到所用电缆的等效相对介电常数与温度的关系曲线如图5所示,结果与已知的ePTFE介电常数的温度变化特性相符。The same method is used to analyze and calculate the equivalent relative dielectric constant at each temperature, and the relationship curve between the equivalent relative dielectric constant of the cable used and temperature is shown in Figure 5. The result is consistent with the known temperature variation characteristics of the ePTFE dielectric constant.
虽然在本文中参照了特定的实施方式来描述本发明,但是应该理解的是,这些实施例仅仅是本发明的原理和应用的示例。因此应该理解的是,可以对示例性的实施例进行许多修改,并且可以设计出其他的布置,只要不偏离所附权利要求所限定的本发明的精神和范围。应该理解的是,可以通过不同于原始权利要求所描述的方式来结合不同的从属权利要求和本文中所述的特征。还可以理解的是,结合单独实施例所描述的特征可以使用在其他所述实施例中。Although the present invention is described herein with reference to specific embodiments, it should be understood that these embodiments are merely examples of the principles and applications of the present invention. It should therefore be understood that many modifications may be made to the exemplary embodiments and that other arrangements may be devised without departing from the spirit and scope of the present invention as defined by the appended claims. It should be understood that the various dependent claims and features described herein may be combined in a manner different from that described in the original claims. It should also be understood that features described in conjunction with individual embodiments may be used in other described embodiments.
Claims (10)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202211613576.6A CN115993485A (en) | 2022-12-15 | 2022-12-15 | Estimation Method of Equivalent Relative Permittivity of Parallel Pair Multi-Core Cables |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202211613576.6A CN115993485A (en) | 2022-12-15 | 2022-12-15 | Estimation Method of Equivalent Relative Permittivity of Parallel Pair Multi-Core Cables |
Publications (1)
Publication Number | Publication Date |
---|---|
CN115993485A true CN115993485A (en) | 2023-04-21 |
Family
ID=85993230
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN202211613576.6A Pending CN115993485A (en) | 2022-12-15 | 2022-12-15 | Estimation Method of Equivalent Relative Permittivity of Parallel Pair Multi-Core Cables |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN115993485A (en) |
-
2022
- 2022-12-15 CN CN202211613576.6A patent/CN115993485A/en active Pending
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US8577632B2 (en) | System and method for identification of complex permittivity of transmission line dielectric | |
CN111308221B (en) | A Characterization Method for Extracting Broadband Continuous Dielectric Properties of Microwave Dielectric Substrates | |
CN111880012B (en) | Method for detecting broadband continuous dielectric characteristic parameters of microwave dielectric substrate | |
Mier et al. | Design and characterization of a magnetic loop antenna for partial discharge measurements in gas insulated substations | |
Al Takach et al. | Two-line technique for dielectric material characterization with application in 3D-printing filament electrical parameters extraction | |
CN106124891B (en) | A kind of planar circuit test space electromagnetic interference method | |
CN113125857A (en) | Wave-absorbing material dielectric parameter measurement and inversion method based on open-circuit coaxial line | |
Shibata | Improvement in liquid permittivity measurement using the cut-off waveguide reflection method | |
Ishibashi et al. | Non-contact PIM evaluation method using a standing wave coaxial tube | |
CN113075460B (en) | Method for testing equivalent dielectric constant and equivalent dielectric loss tangent of communication cable | |
CN109782200A (en) | A method for measuring electromagnetic parameters of materials | |
CN114414958A (en) | A cable insulation aging assessment device and method based on high frequency signal characteristic impedance | |
CN115993485A (en) | Estimation Method of Equivalent Relative Permittivity of Parallel Pair Multi-Core Cables | |
Wang et al. | Modeling of the signal transmission of a coaxial connector with a degraded dielectric layer in a humid environment | |
Marvin et al. | Experimental verification of board level shielding variability at microwave frequencies | |
Sorensen et al. | Design of TEM transmission line for probe calibration up to 40 GHz | |
de Beer et al. | Channel frequency response for a low voltage indoor cable up to 1GHz | |
Cheng et al. | Multifrequency measurements of dielectric properties using a transmission-type overmoded cylindrical cavity | |
JP7370060B2 (en) | Evaluation method, evaluation device, and evaluation system for dielectric materials | |
CN115575720A (en) | Coupling complementary type spiral resonance sensor | |
Obrzut et al. | Input impedance of a coaxial line terminated with a complex gap capacitance-numerical and experimental analysis | |
Hu et al. | Design of an Ultra-Wideband Air-Filled Grounded Coplanar Waveguide for Near-Field Probe Calibration | |
CN116011266B (en) | A method for inverting electrical parameters of long cables using scattering parameters | |
Shin et al. | Extraction of propagation constant of XLPE cable using time-domain transmission | |
Zhuang et al. | An Application of Double-sided Parallel Strip Line Resonator in Dielectric High Frequency Test |
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 |