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CN113190949B - Time domain construction method of CVT (continuously variable transmission) broadband simulation model - Google Patents

Time domain construction method of CVT (continuously variable transmission) broadband simulation model Download PDF

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CN113190949B
CN113190949B CN202011527271.4A CN202011527271A CN113190949B CN 113190949 B CN113190949 B CN 113190949B CN 202011527271 A CN202011527271 A CN 202011527271A CN 113190949 B CN113190949 B CN 113190949B
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司马文霞
杨鸣
王惠
袁涛
孙魄韬
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Abstract

本发明公开一种CVT宽频仿真模型的时域构建方法,步骤包括:1)利用网络分析仪获取CVT的散射参数矩阵S,计算得到CVT的电压传输特性H;2)将电压传输特性H转换为时域的连续状态空间方程;3)将所述连续状态空间方程转换为电路模型,从而得到CVT宽频仿真模型。本发明提出的电容式电压互感器宽频仿真模型的时域构建方法,方法简单,仅需要网络分析仪即可实现对散射参数的测量,解决了当前CVT宽频仿真模型无源修正困难且容易导致精度下降,网络综合后电路元件众多、模型结构复杂等CVT建模难题。

Figure 202011527271

The invention discloses a time-domain construction method of a CVT broadband simulation model. The steps include: 1) using a network analyzer to obtain the scattering parameter matrix S of the CVT, and calculating the voltage transmission characteristic H of the CVT; 2) converting the voltage transmission characteristic H into A continuous state-space equation in the time domain; 3) converting the continuous state-space equation into a circuit model, thereby obtaining a CVT broadband simulation model. The time domain construction method of the capacitive voltage transformer broadband simulation model proposed by the present invention is simple, and only needs a network analyzer to realize the measurement of scattering parameters, which solves the difficulty of passive correction of the current CVT broadband simulation model and easily leads to accuracy After the network is synthesized, there are many circuit components and complex model structure, etc. CVT modeling problems.

Figure 202011527271

Description

一种CVT宽频仿真模型的时域构建方法A Time Domain Construction Method of CVT Wideband Simulation Model

技术领域technical field

本发明涉及电力技术领域,具体是一种CVT宽频仿真模型的时域构建方法。The invention relates to the field of electric power technology, in particular to a method for constructing a CVT broadband simulation model in the time domain.

背景技术Background technique

作为电力系统中重要的一次设备,CVT采用电容分压和电磁单元多级降压的方式得到标准的二次侧电压,不仅具有常规电磁变压器的全部功能,并且有效抑制了与电网中的电容参数匹配造成的铁磁谐振,是电力系统的量测、保护和控制的重要依据。然而,由于CVT结构复杂,应用场景多变,尽管在稳态运行阶段,CVT的二次侧电压仅跟随一次侧信号变化,一旦出现高频暂态,CVT的输出将无法跟随一次侧变化,极易引发继电器的误动作,对基于CVT暂态信号的控制保护和故障定位等造成极大困扰。因此,需建立精确的CVT宽频仿真模型为电力系统分析与保护研究提供基础模型。As an important primary device in the power system, the CVT adopts the method of capacitor voltage division and multi-stage step-down of the electromagnetic unit to obtain the standard secondary side voltage. It not only has all the functions of the conventional electromagnetic transformer, but also effectively suppresses the capacitance parameters in the power grid. The ferromagnetic resonance caused by matching is an important basis for the measurement, protection and control of power systems. However, due to the complex structure of the CVT and the changeable application scenarios, although in the steady state operation stage, the secondary side voltage of the CVT only follows the primary side signal change, once a high frequency transient occurs, the output of the CVT will not be able to follow the change of the primary side. It is easy to cause the malfunction of the relay, and cause great trouble to the control protection and fault location based on the CVT transient signal. Therefore, it is necessary to establish an accurate CVT broadband simulation model to provide a basic model for power system analysis and protection research.

目前,CVT宽频仿真模型的研究主要采用黑盒模型,但是传统黑盒模型结构复杂,且存在微观无源的问题,电路无源会导致模型不稳定,易发散,而无源修正又将导致模型精度降低。因此,需对CVT宽频仿真模型的构建方法进行进一步探索。At present, the research on CVT broadband simulation model mainly adopts the black box model, but the structure of the traditional black box model is complex, and there are micro passive problems, the passive circuit will cause the model to be unstable and easy to diverge, and the passive correction will cause the model Accuracy is reduced. Therefore, it is necessary to further explore the construction method of the CVT broadband simulation model.

发明内容Contents of the invention

本发明的目的是提供一种CVT宽频仿真模型的时域构建方法,包括以下步骤:The object of the present invention is to provide a kind of time domain construction method of CVT broadband simulation model, comprises the following steps:

1)利用网络分析仪获取CVT的散射参数矩阵S,计算得到CVT的电压传输特性H。1) Obtain the scattering parameter matrix S of the CVT by using a network analyzer, and calculate the voltage transmission characteristic H of the CVT.

CVT的散射参数矩阵S如下所示:The scattering parameter matrix S of the CVT is as follows:

Figure BDA0002851186910000011
Figure BDA0002851186910000011

式中,S11、S12、S21、S22表示CVT端口的散射参数。下标1、下标2表示CVT端口序号。In the formula, S 11 , S 12 , S 21 , and S 22 represent the scattering parameters of the CVT port. Subscript 1 and subscript 2 indicate the serial number of the CVT port.

CVT的电压传输特性H如下所示:The voltage transfer characteristic H of the CVT is as follows:

Figure BDA0002851186910000012
Figure BDA0002851186910000012

2)将电压传输特性H转换为时域的连续状态空间方程,步骤包括:2) Converting the voltage transfer characteristic H into a continuous state-space equation in the time domain, the steps include:

2.1)利用矢量匹配法将电压传输特性H拟合为状态空间方程H(s),即:2.1) Use the vector matching method to fit the voltage transfer characteristic H to the state space equation H(s), namely:

H(s)=C(sI-A)-1B+D+sE (3)H(s)=C(sI-A) -1 B+D+sE (3)

式中,A为以极点为对角元素的N阶对角阵。B为N×1阶的单位阵。C为1×N阶的留数矩阵。D、E为常数,拟合过程中通常设置线性项E为0。I为单位向量。s=jω表示拉普拉斯算子。In the formula, A is an N-order diagonal matrix with poles as diagonal elements. B is a unit matrix of order N×1. C is a residue matrix of order 1×N. D and E are constants, and the linear term E is usually set to 0 during the fitting process. I is a unit vector. s=jω represents a Laplacian operator.

2.2)利用反向拉式变换将状态空间方程(3)变换为公式(5)所示的时域的连续状态空间方程,步骤包括:2.2) Utilizing the reverse pull transformation to transform the state-space equation (3) into the continuous state-space equation of the time domain shown in formula (5), the steps include:

2.2.1)设置状态变量x和输出变量如下:2.2.1) Set the state variable x and the output variable as follows:

Figure BDA0002851186910000021
Figure BDA0002851186910000021

式中,u为电压。In the formula, u is the voltage.

2.2.2)根据公式(4),对状态空间方程(3)进行反向拉氏变换,得到时域的连续状态空间方程:2.2.2) According to the formula (4), the state-space equation (3) is reversed to Laplace transform, and the continuous state-space equation in the time domain is obtained:

Figure BDA0002851186910000022
Figure BDA0002851186910000022

式中,k为第k个时刻。xk为第k时刻的状态变量。yk为第k时刻输出电流变量。uk为第k时刻电压变量。x′k为连续性状态变量。In the formula, k is the kth moment. x k is the state variable at the kth moment. y k is the output current variable at the kth moment. u k is the voltage variable at the kth moment. x' k is a continuous state variable.

3)将所述连续状态空间方程转换为电路模型,从而得到CVT宽频仿真模型,步骤包括:3) converting the continuous state space equation into a circuit model, thereby obtaining a CVT broadband simulation model, the steps include:

3.1)利用中心差分法对连续状态空间方程进行离散化,得到:3.1) Using the central difference method to discretize the continuous state space equation, we get:

Figure BDA0002851186910000023
Figure BDA0002851186910000023

式中,h是采样时长。xk+1为第k+1时刻的状态变量。uk+1为第k+1时刻电压变量。yk+1为第k+1时刻输出电流变量。In the formula, h is the sampling time. x k+1 is the state variable at the k+1th moment. u k+1 is the voltage variable at the k+1th moment. y k+1 is the output current variable at the k+1th moment.

3.2)对公式(6)进行化简,得到:3.2) Formula (6) is simplified to obtain:

Figure BDA0002851186910000024
Figure BDA0002851186910000024

其中,向量α、向量μ分别如下所示:Among them, vector α and vector μ are as follows:

α=(2I-Ah)-1(2I+Ah) (8)α=(2I-Ah) -1 (2I+Ah) (8)

μ=(2I-Ah)-1h (9)μ=(2I-Ah) -1 h (9)

3.3)修正状态变量为:3.3) The modified state variable is:

Figure BDA0002851186910000031
Figure BDA0002851186910000031

式中,

Figure BDA0002851186910000032
为k+1时刻状态变量修正值。In the formula,
Figure BDA0002851186910000032
is the corrected value of the state variable at time k+1.

3.4)将公式(10)代入公式(7)中,得到:3.4) Substitute formula (10) into formula (7) to get:

Figure BDA0002851186910000033
Figure BDA0002851186910000033

式中,

Figure BDA0002851186910000034
为k时刻状态变量修正值。In the formula,
Figure BDA0002851186910000034
is the corrected value of the state variable at time k.

其中,单位矩阵

Figure BDA0002851186910000035
矩阵G如下所示:Among them, the identity matrix
Figure BDA0002851186910000035
The matrix G looks like this:

Figure BDA0002851186910000036
Figure BDA0002851186910000036

G=D+CμB (13)G=D+CμB (13)

3.4)令输出向量

Figure BDA0002851186910000037
更新公式(11),得到CVT宽频仿真模型:3.4) Let the output vector
Figure BDA0002851186910000037
Update formula (11) to get the CVT broadband simulation model:

Figure BDA0002851186910000038
Figure BDA0002851186910000038

式中,is,k为k时刻时域电流向量。ys,k+1为k+1时刻时域输出向量。In the formula, i s,k is the time-domain current vector at time k. y s,k+1 is the time domain output vector at time k+1.

本发明的技术效果是毋庸置疑的,本发明提出的电容式电压互感器宽频仿真模型的时域构建方法,方法简单,仅需要网络分析仪即可实现对散射参数的测量,解决了当前CVT宽频仿真模型无源修正困难且容易导致精度下降,网络综合后电路元件众多、模型结构复杂等CVT建模难题。The technical effect of the present invention is unquestionable. The time domain construction method of the capacitive voltage transformer broadband simulation model proposed by the present invention is simple, and only a network analyzer is needed to realize the measurement of scattering parameters, which solves the problem of the current CVT broadband simulation model. Passive correction of the simulation model is difficult and easily leads to a decrease in accuracy. After network synthesis, there are many circuit components and complex model structures. CVT modeling problems.

附图说明Description of drawings

图1为散射参数测量示意图;Figure 1 is a schematic diagram of scattering parameter measurement;

图2为电压传输函数拟合结果;Fig. 2 is the fitting result of voltage transfer function;

图3为诺顿等价结构;Figure 3 is the Norton equivalent structure;

图4为雷电冲击电压实验波形Figure 4 is the experimental waveform of lightning impulse voltage

图5为CVT实测雷电电压波形与仿真结果对比;Figure 5 shows the comparison between the measured lightning voltage waveform of the CVT and the simulation results;

图6为方法流程图。Figure 6 is a flowchart of the method.

具体实施方式Detailed ways

下面结合实施例对本发明作进一步说明,但不应该理解为本发明上述主题范围仅限于下述实施例。在不脱离本发明上述技术思想的情况下,根据本领域普通技术知识和惯用手段,做出各种替换和变更,均应包括在本发明的保护范围内。The present invention will be further described below in conjunction with the examples, but it should not be understood that the scope of the subject of the present invention is limited to the following examples. Without departing from the above-mentioned technical ideas of the present invention, various replacements and changes made according to common technical knowledge and conventional means in this field shall be included in the protection scope of the present invention.

实施例1:Example 1:

参见图1至图6,一种CVT(电容式电压互感器)宽频仿真模型的时域构建方法,包括以下步骤:Referring to Fig. 1 to Fig. 6, a kind of time-domain construction method of CVT (capacitive voltage transformer) broadband simulation model comprises the following steps:

1)利用网络分析仪获取CVT的散射参数矩阵S,计算得到CVT的电压传输特性H。CVT宽频仿真模型的时域构建方法用于建立电容式电压互感器宽频时域电路模型。1) Obtain the scattering parameter matrix S of the CVT by using a network analyzer, and calculate the voltage transmission characteristic H of the CVT. The time-domain construction method of CVT broadband simulation model is used to establish the broadband time-domain circuit model of capacitive voltage transformer.

CVT的散射参数矩阵S如下所示:The scattering parameter matrix S of the CVT is as follows:

Figure BDA0002851186910000041
Figure BDA0002851186910000041

式中,S11、S12、S21、S22表示CVT端口的散射参数。下标1、下标2表示CVT端口序号。In the formula, S 11 , S 12 , S 21 , and S 22 represent the scattering parameters of the CVT port. Subscript 1 and subscript 2 indicate the serial number of the CVT port.

CVT的电压传输特性H如下所示:The voltage transfer characteristic H of the CVT is as follows:

Figure BDA0002851186910000042
Figure BDA0002851186910000042

2)将电压传输特性H转换为时域的连续状态空间方程,步骤包括:2) Converting the voltage transfer characteristic H into a continuous state-space equation in the time domain, the steps include:

2.1)利用矢量匹配法将电压传输特性H拟合为状态空间方程,即H(s):2.1) Use the vector matching method to fit the voltage transfer characteristic H to the state space equation, namely H(s):

H(s)=C(sI-A)-1B+D+sE (3)H(s)=C(sI-A) -1 B+D+sE (3)

式中,A为以极点为对角元素的N阶对角阵。B为N×1阶的单位阵。C为1×N阶的留数矩阵。D、E为常数,拟合过程中通常设置线性项E为0。I为单位向量。s表示拉普拉斯算子,s=jωIn the formula, A is an N-order diagonal matrix with poles as diagonal elements. B is a unit matrix of order N×1. C is a residue matrix of order 1×N. D and E are constants, and the linear term E is usually set to 0 during the fitting process. I is a unit vector. s represents the Laplacian operator, s=jω

2.2)利用反向拉式变换将状态空间方程(3)变换为式(5)所示的时域的连续状态空间方程,步骤如下:2.2) Utilize the inverse pull transformation to transform the state-space equation (3) into the continuous state-space equation in the time domain shown in formula (5), the steps are as follows:

令:make:

Figure BDA0002851186910000043
Figure BDA0002851186910000043

式中,u为电压。In the formula, u is the voltage.

通过反向拉氏变换,得到时域的连续状态空间方程:By inverse Laplace transform, the continuous state-space equation in the time domain is obtained:

Figure BDA0002851186910000044
Figure BDA0002851186910000044

式中,k为第k个时刻。xk为第k时刻的状态变量。yk为第k时刻输出电流变量。uk为第k时刻电压变量。x′k为连续性状态变量。In the formula, k is the kth moment. x k is the state variable at the kth moment. y k is the output current variable at the kth moment. u k is the voltage variable at the kth moment. x' k is a continuous state variable.

3)将所述连续状态空间方程转换为电路模型,从而得到CVT宽频仿真模型,步骤包括:3) converting the continuous state space equation into a circuit model, thereby obtaining a CVT broadband simulation model, the steps include:

3.1)利用中心差分法对连续状态空间方程进行离散化,得到:3.1) Using the central difference method to discretize the continuous state space equation, we get:

Figure BDA0002851186910000051
Figure BDA0002851186910000051

式中,h是采样时长。xk+1为第k+1时刻的状态变量。uk+1为第k+1时刻电压变量。yk+1为第k+1时刻输出电流变量。In the formula, h is the sampling time. x k+1 is the state variable at the k+1th moment. u k+1 is the voltage variable at the k+1th moment. y k+1 is the output current variable at the k+1th moment.

3.2)对公式(6)进行化简,得到:3.2) Formula (6) is simplified to obtain:

Figure BDA0002851186910000052
Figure BDA0002851186910000052

其中,向量α、向量μ分别如下所示:Among them, vector α and vector μ are as follows:

α=(2I-Ah)-1(2I+Ah) (8)α=(2I-Ah) -1 (2I+Ah) (8)

μ=(2I-Ah)-1h (9)μ=(2I-Ah) -1 h (9)

3.3)修正状态变量为:3.3) The modified state variable is:

Figure BDA0002851186910000053
Figure BDA0002851186910000053

式中,

Figure BDA0002851186910000054
为k+1时刻状态变量修正值。In the formula,
Figure BDA0002851186910000054
is the corrected value of the state variable at time k+1.

3.4)将公式(10)代入公式(7)中,得到:3.4) Substitute formula (10) into formula (7) to get:

Figure BDA0002851186910000055
Figure BDA0002851186910000055

式中,

Figure BDA0002851186910000056
为k时刻状态变量修正值。In the formula,
Figure BDA0002851186910000056
is the corrected value of the state variable at time k.

其中,单位矩阵

Figure BDA0002851186910000057
矩阵G如下所示:Among them, the identity matrix
Figure BDA0002851186910000057
The matrix G looks like this:

Figure BDA0002851186910000058
Figure BDA0002851186910000058

G=D+CμB (13)G=D+CμB (13)

3.4)令输出向量

Figure BDA0002851186910000059
更新公式(11),得到CVT宽频仿真模型:3.4) Let the output vector
Figure BDA0002851186910000059
Update formula (11) to get the CVT broadband simulation model:

Figure BDA00028511869100000510
Figure BDA00028511869100000510

式中,is,k为k时刻时域电流向量。ys,k+1为k+1时刻时域输出向量。In the formula, i s,k is the time-domain current vector at time k. y s,k+1 is the time domain output vector at time k+1.

CVT宽频仿真模型(14)用于反映CVT运行状态。The CVT broadband simulation model (14) is used to reflect the CVT running state.

实施例2:Example 2:

一种CVT(电容式电压互感器)宽频仿真模型的时域构建方法,包括以下步骤:A time-domain construction method of a CVT (capacitive voltage transformer) broadband simulation model, comprising the following steps:

1)利用网络分析仪获取CVT的散射参数矩阵S,计算得到CVT的电压传输特性H。1) Obtain the scattering parameter matrix S of the CVT by using a network analyzer, and calculate the voltage transmission characteristic H of the CVT.

由散射参数计算宽频电压传输函数的具体方法为:The specific method to calculate the broadband voltage transfer function from the scattering parameters is as follows:

将CVT看作一个二端口网络,利用网络分析仪E5061B获取CVT的散射参数矩阵S,计算得到CVT的电压传输函数,公式为:Consider the CVT as a two-port network, use the network analyzer E5061B to obtain the scattering parameter matrix S of the CVT, and calculate the voltage transfer function of the CVT, the formula is:

Figure BDA0002851186910000061
Figure BDA0002851186910000061

Figure BDA0002851186910000062
Figure BDA0002851186910000062

2)采用矢量匹配法和反向拉式变换将电压传输特性H拟合转换为时域的状态空间方程形式。2) The voltage transfer characteristic H is fitted and transformed into a state-space equation in the time domain by vector matching method and reverse pull transformation.

采用矢量匹配法将电压传输函数拟合为状态空间方程形式,公式为:The voltage transfer function is fitted to the form of state space equation by vector matching method, the formula is:

H(s)=C(sI-A)-1B+D+sEH(s)=C(sI-A) -1 B+D+sE

令:make:

Figure BDA0002851186910000063
Figure BDA0002851186910000063

通过反向拉式变换,将上式变换为时域的连续状态空间方程:Through the reverse pull transformation, the above equation is transformed into a continuous state space equation in the time domain:

Figure BDA0002851186910000064
Figure BDA0002851186910000064

式中,k为第k个时刻。xk为第k时刻的状态变量。yk为第k时刻输出电流变量。uk为第k时刻电压变量。In the formula, k is the kth moment. x k is the state variable at the kth moment. y k is the output current variable at the kth moment. u k is the voltage variable at the kth moment.

其中,A为以极点为对角元素的N阶对角阵。B为N×1阶的单位阵。C为1×N阶的留数矩阵。D、E为常数。在矢量匹配过程中,线性项一般为0,所以可令E=0。Among them, A is an N-order diagonal matrix with poles as diagonal elements. B is a unit matrix of order N×1. C is a residue matrix of order 1×N. D and E are constants. In the process of vector matching, the linear item is generally 0, so E=0 can be set.

3)通过离散状态方程和诺顿等价将数学模型转换为电路模型,建立精确的CVT宽频仿真模型。3) Convert the mathematical model into a circuit model through the discrete state equation and Norton equivalent, and establish an accurate CVT broadband simulation model.

所述宽频导纳模型构建的具体方法为:The concrete method of described broadband admittance model construction is:

采用中心差分法对连续状态空间方程进行离散化,将离散状态方程等价为一个带诺顿等效的电流源的结构Using the central difference method to discretize the continuous state space equation, the discrete state equation is equivalent to a current source structure with Norton equivalent

Figure BDA0002851186910000071
Figure BDA0002851186910000071

其中,h是采样时长。Among them, h is the sampling time.

进一步化简得到:Simplify further to get:

Figure BDA0002851186910000072
Figure BDA0002851186910000072

其中:in:

α=(2I-Ah)-1(2I+Ah)α=(2I-Ah) -1 (2I+Ah)

μ=(2I-Ah)-1hμ=(2I-Ah) -1 h

令:make:

Figure BDA0002851186910000073
Figure BDA0002851186910000073

则:but:

Figure BDA0002851186910000074
Figure BDA0002851186910000074

其中:in:

Figure BDA0002851186910000075
Figure BDA0002851186910000075

G=D+CμBG=D+CμB

令:make:

Figure BDA0002851186910000076
Figure BDA0002851186910000076

则:but:

Figure BDA0002851186910000077
Figure BDA0002851186910000077

实施例3:Example 3:

应用基于离散状态方程的电容式电压互感器宽频仿真模型构建方法的实验,步骤包括:The experiment of applying the method of constructing the broadband simulation model of capacitive voltage transformer based on the discrete state equation, the steps include:

1)选用一台额定电压

Figure BDA0002851186910000078
准确级为:0.2/0.5/3P,额定容量为10/10/10VA,额定变比为350:1的电容式电压互感器,利用上述方法测量和获取CVT的宽频仿真模型参数和结构。1) Select a rated voltage
Figure BDA0002851186910000078
Accuracy class: 0.2/0.5/3P, rated capacity 10/10/10VA, rated transformation ratio 350:1 capacitive voltage transformer, use the above method to measure and obtain the CVT broadband simulation model parameters and structure.

2)根据图1所示搭建实验平台,将CVT看作一个二端口网络,采用网络分析仪E5061B,获取5Hz~1MHz内服从对数分布的4801个频率点及其相应的散射参数S,计算得到CVT的宽频电压传输函数H。2) According to the experimental platform shown in Figure 1, the CVT is regarded as a two-port network, and the network analyzer E5061B is used to obtain 4801 frequency points that obey the logarithmic distribution within 5 Hz to 1 MHz and the corresponding scattering parameters S, and calculate CVT broadband voltage transfer function H.

3)采用矢量匹配法和反向拉式变换对电压传输特性H进行拟合和转换,结果如图2所示,图中实线为实测CVT低压侧电压波形,虚线为仿真CVT低压侧电压波形。图2、4、5中所有电压幅值均以输入电压为基准进行归一化处理。3) The voltage transfer characteristic H is fitted and converted by vector matching method and reverse pull transformation. The results are shown in Figure 2. The solid line in the figure is the measured voltage waveform on the low-voltage side of the CVT, and the dashed line is the voltage waveform on the simulated CVT low-voltage side. . All voltage amplitudes in Figures 2, 4, and 5 are normalized based on the input voltage.

通过离散化状态方程和诺顿等价将CVT宽频导纳数学模型转换为如图3所示的宽频导纳电路模型,建立精确的CVT宽频仿真模型。By discretizing the state equation and Norton equivalent, the CVT broadband admittance mathematical model is converted into a broadband admittance circuit model as shown in Figure 3, and an accurate CVT broadband simulation model is established.

4)根据以上数据,搭建CVT宽频仿真模型电路,在CVT高压侧施加如图4所示的雷电冲击电压波形。同时,将该波形作为模型输入信号,施加到本文建立的CVT宽频仿真模型中,低压侧电压波形实测和仿真结果图5所示,图中实线为实测CVT低压侧电压波形,虚线为仿真CVT低压侧电压波形。计算得到,CVT宽频仿真模型首峰值误差为3.31%,表明CVT宽频仿真模型能准确表示CVT的高频电压传输特性。4) According to the above data, build a CVT broadband simulation model circuit, and apply the lightning impulse voltage waveform shown in Figure 4 on the high voltage side of the CVT. At the same time, the waveform is used as the model input signal and applied to the CVT broadband simulation model established in this paper. The measured and simulated results of the low-voltage side voltage waveform are shown in Figure 5. The solid line in the figure is the measured CVT low-voltage side voltage waveform, and the dotted line is the simulated CVT Low voltage side voltage waveform. It is calculated that the first peak error of the CVT broadband simulation model is 3.31%, which indicates that the CVT broadband simulation model can accurately represent the high-frequency voltage transmission characteristics of the CVT.

Claims (2)

1. A time domain construction method of a CVT broadband simulation model is characterized by comprising the following steps:
1) Acquiring a scattering parameter matrix S of the CVT by using a network analyzer, and calculating to obtain a voltage transmission characteristic H of the CVT;
the voltage transfer characteristic H of the CVT is as follows:
Figure FDA0004054345190000011
in the formula, S 11 、S 12 、S 21 、S 22 A scattering parameter indicative of a CVT port; subscript 1 and subscript 2 represent CVT port serial numbers;
2) Converting the voltage transmission characteristic H into a continuous state space equation of a time domain;
the step of converting the voltage transfer characteristic H into a continuous state space equation in the time domain comprises:
2.1 Using a vector matching method to fit the voltage transfer characteristic H to a state space equation H(s), i.e.:
H(s)=C(sI-A) -1 B+D+sE (2)
in the formula, A is an N-order diagonal matrix taking poles as diagonal elements; b is a unit array of Nx 1 order; c is a residue matrix of 1 XN order; D. e is a constant; i is a unit vector; s = j ω represents the laplacian operator;
2.2 Transforming the state space equation (2) into a time domain continuous state space equation as shown in equation (3) using an inverse pull transform, comprising the steps of:
2.2.1 Set state variable x and output variable y as follows:
Figure FDA0004054345190000012
wherein u is a voltage;
2.2.2 Inverse Laplace transform is performed on the state space equation (2) according to the formula (3) to obtain a continuous state space equation of the time domain:
Figure FDA0004054345190000013
in the formula, k is the kth moment; x is the number of k Is a state variable at the kth moment; y is k Outputting a current variable for the kth moment; u. u k Is the voltage variable at the kth moment; x' k Is a continuity state variable;
3) Converting the continuous state space equation into a circuit model so as to obtain a CVT broadband simulation model;
the step of converting the continuous state space equations into a circuit model comprises:
3.1 Discretizing a continuous state space equation by using a central difference method to obtain:
Figure FDA0004054345190000021
wherein h is the sampling duration; x is a radical of a fluorine atom k+1 The state variable at the k +1 th moment; u. of k+1 Voltage variable at the k +1 th moment; y is k+1 Outputting a current variable for the k +1 th moment;
3.2 Simplifying equation (5) to obtain:
Figure FDA0004054345190000022
wherein, the vector α and the vector μ are respectively as follows:
α=(2I-Ah) -1 (2I+Ah) (7)
μ=(2I-Ah) -1 h (8)
3.3 Modified state variables are:
Figure FDA0004054345190000023
in the formula (I), the compound is shown in the specification,
Figure FDA0004054345190000024
correcting state variables for time k +1A value;
3.4 Substituting equation (9) into equation (6) yields:
Figure FDA0004054345190000025
in the formula (I), the compound is shown in the specification,
Figure FDA0004054345190000026
a state variable correction value at the time k;
wherein the identity matrix
Figure FDA0004054345190000027
Matrix G is as follows:
Figure FDA0004054345190000028
G=D+CμB (12)
3.5 Order output vector
Figure FDA0004054345190000029
And (5) updating the formula (10) to obtain a CVT broadband simulation model:
Figure FDA00040543451900000210
in the formula i s,k Time domain current vector at the k moment; y is s,k+1 The time domain output vector is at the moment k + 1.
2. The time domain construction method of the CVT wideband simulation model according to claim 1, characterized in that a scattering parameter matrix S of the CVT is as follows:
Figure FDA0004054345190000031
in the formula, S 11 、S 12 、S 21 、S 22 A scattering parameter indicative of a CVT port; subscript 1 and subscript 2 denote CVT port number.
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