外文翻译--基于优化的牛顿—拉夫逊法和牛顿法的潮流计算

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牛顿拉夫逊法计算潮流步骤

牛顿拉夫逊法计算潮流步骤

牛顿拉夫逊法计算潮流步骤牛顿拉夫逊法(Newton-Raphson method)是一种用于求解非线性方程组的迭代方法,它可以用来计算电力系统潮流的解。

潮流计算是电力系统规划和运行中的重要任务,它的目标是求解电力系统中各节点的电压幅值和相角,以及线路的功率流向等参数,用于分析电力系统的稳定性和安全性,以及进行电力系统规划和调度。

下面是使用牛顿拉夫逊法计算潮流的一般步骤:步骤1:初始化首先,需要对电力系统的各个节点(包括发电机节点和负荷节点)的电压幅值和相角进行初始化,一般可以使用其中一种估计值或者历史数据作为初始值。

步骤2:建立潮流方程根据电力系统的潮流计算模型,可以建立节点电压幅值和相角的平衡方程,一般采用节点注入功率和节点电压的关系来表示。

潮流方程一般是一个非线性方程组,包含了各个节点之间的复杂关系。

步骤3:线性化方程组将潮流方程组进行线性化处理,一般采用泰勒展开的方法,将非线性方程组变为线性方程组。

线性化的过程需要计算雅可比矩阵,即方程组中的系数矩阵。

步骤4:求解线性方程组利用线性方程组的求解方法,比如高斯消元法或LU分解法等,求解线性方程组,得到电压幅值和相角的修正量。

步骤5:更新节点电压根据线性方程组的解,更新各个节点的电压幅值和相角,得到新的节点电压。

步骤6:检查收敛性判断节点电压的修正量是否小于设定的收敛阈值,如果满足收敛条件,则停止迭代;否则,返回步骤3,循环进行线性化方程组和线性方程组的求解。

步骤7:输出结果当潮流计算收敛时,输出最终的节点电压幅值和相角,以及线路的功率流向等参数。

牛顿拉夫逊法是一种高效、快速且收敛性良好的方法,广泛应用于电力系统潮流计算。

在实际应用中,可能会遇到多次迭代或者收敛性不好的情况,此时可以采用退火技术或其他优化算法进行改进。

此外,牛顿拉夫逊法的计算也可以并行化,利用多核处理器或者分布式计算集群来加速计算过程。

总之,牛顿拉夫逊法是一种重要的潮流计算方法,通过迭代计算逼近非线性方程组的解,可以得到电力系统中各节点的电压幅值和相角,用于分析电力系统的稳定性和安全性。

潮流计算-英文文献

潮流计算-英文文献

外文资料Summary of power flow calculationPower system is calculated on the trend of steady-state operation of the power system as a basis, it's running under the given conditions and determine the entire system wiring in various parts of the power system running: the voltage of the bus, all components of a mid-stream power, The power loss, and so on. Power system planning in the design and operation of the existing power system in the form of research, we need to calculate the trend of using quantitative analysis of comparative power programme or operation mode is reasonable. Reliability and economy. In addition, the power flow calculation is calculated static and dynamic stability of the foundation of stability. So the trend is calculated on the power system of a very important and very basis of calculation. Power flow calculation also divided into offline and online calculation of two terms, the former mainly used for system planning and design and organization of the operation mode, while the latter is running for the system of regular monitoring and real-time control. The use of electronic digital computer to calculate the trend of the power system from the mid-1950s has already begun. Power flow problems in mathematical calculation is a group of diverse non-linear equations to solve the problem, its solution can not be separated from iteration. Therefore, the flow calculation method, it requires first and foremost a reliable convergence, and give the correct answers. As the power system structure and parameters of some of the features, and with the continuous expansion of the power system, the trend of increasing order of the equation, so the formula is not any mathematical method can guarantee is given the correct answer. This calculation of the power system to become a staff continue to seek new and more reliable way of the important factors.Use of digital computers in the power flow problems at the beginning, the general adoption of a node admittance matrix-based successive into the law. The principle of this method is relatively simple to compare the volume of digital computer memory, to the 1950s computer manufacturing level and then the power system theoretical level. However, it is convergence of the poor, when the system large-scale change, the sharp rise in the number of iteration in the calculation of convergence are often not the case iteration. This forced the staff to the power system to calculate impedance matrix-based successive into the law. Impedance method to improve the flow of the convergence of computing, the solution of the admittance system can not solve some of the trend, in the 1960s, access to a wide range of applications, has the power system design. Operational and research has made great contribution. At present, there are stillsome in the power industry units impedance method to calculate the trend. Impedance of the main shortcomings of the occupation of the computer's memory, each iteration of the large amount of calculation. When the system continue to expand, the more prominent of these shortcomings. 16 K memory of a computer in the use of impedance method can only be calculated at 100 following the system, 32 K memory of the computer can only calculate 150 nodes under the system. In this way, many of the power system in order to use impedance method shall not be first on the trend of the system is the streamlining of work. In order to overcome resistance in memory and speed of the shortcomings of the mid-1960s to the development of the impedance matrix-based Block impedance. This approach to a large-scale system divided into several small regional system, the computer only need to store various parts of the system impedance matrix contact line between them and the resistance, not only substantial savings in memory capacity, but also improve the Computing speed.Overcome the shortcomings of the impedance of hungry is another way to use Newton - Raphson method. This is the mathematics of nonlinear equations to solve the typical method, a better convergence. In resolving the issue of power flow calculation, is admittance matrix-based, therefore, as long as we can in the iterative process as much as possible to maintain the formula coefficient matrix sparse, and can greatly improve Newton's Law trend of the efficiency of procedures . Since the mid-1960s, Newton's law in the use of the best order of elimination, the Newton in convergence. Memory requirements. Speed all over the impedance, as the late 1960s after the widespread adoption of the excellent way.Flow calculation flexibility and convenience of the request, the application of digital computers is also a very key issue. In the past for a long time, the power flow calculation relies on the Taiwan exchange. Taiwan simulates the exchange of power systems, computing platforms in the calculation of the trend of the exchange, calculated at any time surveillance systems can run different parts of the state to meet requirements, if they run certain parts of unreasonable, you can make adjustments immediately. In this way, the equivalent of the process on the computing staff lost operating system. Adjustment process is very intuitive, physical concept is very clear. When the use of digital computers to calculate the trend when it lost this visual. To make up for this shortcoming, the trend of the establishment of procedures to the extent possible, in terms of computer calculation in the process of strengthening the process of the computer monitor and control, and to facilitate a variety of modifications and adjustments. Power flow calculation is not a simple calculation, to run it as a form of adjustment may be more precise. In order to get a reasonable run, often need to keep in accordance with the results, modify the original data. In this sense, the trend in the preparation of our program, the ease of use and flexibility must be sufficient attention. Therefore, in addition to the requirements in various ways to modify as muchas possible. Adjustment, we must pay attention to input and output of convenience and flexibility, strengthening human-computer links, so that the calculation of staff to monitor timely and appropriate calculations to control the conduct of calculation .Power flow calculation is a power system analysis of the most basic terms, the complex power system under normal and failure conditions steady-state running the calculation. The trend is calculated to strike a target in the power system to be running the calculation. That is, voltage and power distribution node, to check whether the components of the system overload. Voltage meets all requirements of the distribution and allocation of power is reasonable and the power loss, and so on. Of the existing power system operations and expansion, the new power system planning and design of the power system for static and transient stability of the trend are calculated as the basis. If the trend of the results available on steady-state power system, or estimate the optimal security, such as the trend of the flow calculation method and the model has a direct impact. The actual power system that the main trend of technology adoption Newton - Raphson method.In the management of the operation mode, the trend of power grid operation mode is to determine the basic starting point in planning areas, the need for trend analysis verified the reasonableness of the plan in real-time operating environment, dispatchers, provided the trend of End-expected operating conditions in the power grid To check the trend of operational reliability. In the power system dispatching a number of areas related to the trend of grid computing. Electricity network is to determine the trend of running the basic factors, the trend is steady-state power system on the basis and prerequisite .外文原文翻译电力系统潮流计算综述电力系统潮流计算是研究电力系统稳态运行情况的一种计算,它根据给定的运行条件及系统接线情况确定整个电力系统各部分的运行状态:各母线的电压,各元件中流过的功率,系统的功率损耗等等。

牛顿拉夫逊法潮流计算

牛顿拉夫逊法潮流计算

牛顿拉夫逊法潮流计算牛顿-拉夫逊法(Newton-Raphson method)是一种用于求解非线性方程的数值方法。

它通过迭代逼近根的方式,将非线性方程转化为一系列的线性方程来求解。

在电力系统中,潮流计算用于确定电力网中节点的电压幅值和相角。

潮流计算是电力系统分析的重要基础,可以用于计算电力系统的潮流分布、功率损耗、节点电压稳定度等参数,为电力系统的规划、运行和控制提供参考依据。

牛顿-拉夫逊法是一种常用的潮流计算方法,它的基本思想是通过不断迭代来逼近电网的潮流分布,直到满足一定的收敛条件。

下面将对牛顿-拉夫逊法的具体步骤进行详细介绍。

首先,我们需要建立电力网络的节点潮流方程,即功率方程。

对于每一个节点i,其节点功率方程可以表示为:Pi - Vi * (sum(Gij * cos(θi - θj)) - sum(Bij * sin(θi -θj))) = 0Qi - Vi * (sum(Gij * sin(θi - θj)) + sum(Bij * cos(θi -θj))) = 0其中,Pi和Qi分别为节点i的有功功率和无功功率,Vi和θi分别为节点i的电压幅值和相角,Gij和Bij分别为节点i和节点j之间的导纳和电纳。

接下来,我们需要对每个节点的电压幅值和相角进行初始化。

一般情况下,可以将电压幅值设置为1,相角设置为0。

然后,我们可以开始进行迭代计算。

在每一轮迭代中,我们需要计算每个节点的雅可比矩阵和功率残差,然后更新电压幅值和相角。

雅可比矩阵可以通过对节点功率方程进行求导得到,具体如下:dPi/dVi = -sum(Vj * (Gij * sin(θi - θj) + Bij * cos(θi - θj)))dPi/dθi = sum(Vj * (Gij * Vi * cos(θi - θj) - Bij * Vi * sin(θi - θj)))dQi/dVi = sum(Vj * (Gij * cos(θi - θj) - Bij * sin(θi - θj)))dQi/dθi = sum(Vj * (Gij * Vi * sin(θi - θj) + Bij * Vi * cos(θi - θj)))功率残差可以通过将节点功率方程代入得到,如下:RPi = Pi - Vi * (sum(Gij * cos(θi - θj)) - sum(Bij *sin(θi - θj)))RQi = Qi - Vi * (sum(Gij * sin(θi - θj)) + sum(Bij *cos(θi - θj)))最后,我们可以使用牛顿-拉夫逊法的迭代公式来更新电压幅值和相角,具体如下:Vi(new) = Vi(old) + ΔViθi(new) = θi(old) + Δθi其中,ΔVi和Δθi分别为通过求解线性方程组得到的电压幅值和相角的增量。

基于MATLAB的牛顿拉夫逊法电力潮流计算与实现

基于MATLAB的牛顿拉夫逊法电力潮流计算与实现

作者简介 罗杰(1978—),男,硕士,华东交通大学讲师,从事电力
自动化系统的研究和教学工作。
184


(Department of Electrical and Electronic Engineering, East China Jiaotong University,

Jiangxi Nanchang 330013))



摘 要:牛顿 - 拉夫逊法是电力系统潮流计算最常用的算法之一,它收敛性好,迭代次数较少。本文基于牛顿 - 拉夫逊
system. It has good convergence and less iterative number. The paper gives a specific analysis of New-
ton-Raphson method, designs a visual interface based on MATLAB.The visual interface has a good operability
1 电力潮流计算方法的发展 最初,电力系统潮流计算是通过人工计算的。后来为了
适应电力系统日益发展的需要,采用了交流计算台。随着电 子数字计算机的出现,1956 年 Ward 等人编制了实际可行的 计算机潮流计算程序。这样,就为日趋复杂的大规模电力系 统提供了极其有力的计算手段。经过几十年的发展,电力系 统潮流计算已经十分成熟。电力系统潮流计算形式分为离线 计算和在线计算两种。前者主要用于电力系统规划设计、安 排系统的运行方式;后者则用于正在运行系统的实时监视和 实时控制。在计算原理上离线和在线潮流计算是相同的,都 要求满足以下几点:
表二 迭代过程中雅可比矩阵的各对角元素

基于改进牛顿法的VSC-HVDC潮流计算

基于改进牛顿法的VSC-HVDC潮流计算

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牛顿拉斐逊法潮流计算

牛顿拉斐逊法潮流计算

牛顿拉斐逊法潮流计算牛顿拉夫逊法(Newton-Raphson method)是一种数值计算方法,用于解非线性方程。

其原理是通过迭代来逼近方程的根。

在电力系统中,牛顿拉夫逊法常用于求解潮流计算问题。

潮流计算是电力系统调度运行和规划的基础工作,其目的是确定电力系统各节点的电压幅值和相角,以及各支线上的功率和无功功率。

通过潮流计算可以有效地评估电力系统的稳定性和运行状态,并为电力系统的调度和规划提供参考依据。

牛顿拉夫逊法的核心思想是通过接近方程的根来求解非线性方程。

其基本步骤如下:1.初始化:选取一个初始点作为方程的近似解,通常选择电力系统的平衡状态作为初值。

2.构造雅可比矩阵:根据潮流方程的特点,建立牛顿拉夫逊法的雅可比矩阵。

雅可比矩阵描述了非线性方程的导数关系,用于迭代计算过程中的线性化。

3.迭代计算:利用雅可比矩阵和当前解向量,构建迭代格式,并计算得到新的解向量。

迭代格式中,包括牛顿方程和拉夫逊方程。

牛顿方程用于计算不平衡功率的校正量,而拉夫逊方程用于计算不平衡电压的校正量。

4.收敛判断:判断迭代计算得到的新解是否满足收敛条件。

通常使用误差向量的范数作为判断依据。

如果误差向量的范数小于预先设定的阈值,即可认为迭代已经收敛。

5.循环迭代:如果迭代计算得到的新解不满足收敛条件,继续进行迭代计算,直到达到收敛条件为止。

牛顿拉夫逊法的优点是收敛速度较快,尤其适用于求解非线性方程的问题。

然而,该方法也存在一些缺点。

首先,牛顿拉夫逊法需要提供一个合适的初始点,如果初始点选择不当,可能会导致迭代过程发散。

其次,构造雅可比矩阵和计算迭代格式的过程较为复杂,需要一定的数学基础和计算能力。

在电力系统潮流计算中,牛顿拉夫逊法广泛应用于求解节点电压和支路功率的平衡方程。

通过牛顿拉夫逊法,可以准确地计算出系统各节点的电压幅值和相角,指导电网的调度运营和规划工作。

总之,牛顿拉夫逊法是一种重要的数值计算方法,特别适用于求解非线性方程。

第三节牛顿拉夫逊法潮流计算

第三节牛顿拉夫逊法潮流计算

第三节牛顿拉夫逊法潮流计算牛顿-拉夫逊法(Newton-Raphson method)是一种数值计算方法,用于求解非线性方程和潮流计算问题。

它是基于牛顿迭代法和拉夫逊迭代法的结合,可高效地求解电力系统潮流计算问题。

潮流计算是电力系统运行分析中的重要环节,其目标是确定系统中每个节点的电压和相角,并计算各个支路的电流,以评估系统的功率传输和稳定性。

在传统的高压电力系统中,由于负荷、发电机和传输线等元件的非线性特性,潮流计算问题呈现为非线性的数学方程组,通常采用迭代方法求解。

牛顿-拉夫逊法的基本思想是通过对方程组的线性化近似,迭代求解线性方程组的解,以接近方程组的精确解。

它通过将非线性方程组转化为以下形式进行迭代:F(x)=0其中,F(x)是非线性方程组的向量函数,x是未知向量。

牛顿-拉夫逊法的迭代过程可通过以下步骤进行:1.初始化变量:根据系统的初始状态进行节点电压和相角的初始化。

2.计算雅可比矩阵:通过对非线性方程组进行偏导,得到雅可比矩阵。

雅可比矩阵描述了各个节点潮流量与节点电压和相角之间的关系。

3.迭代计算:通过牛顿迭代法进行迭代计算,直到达到指定的收敛条件。

具体步骤为:a.解线性方程组:根据雅可比矩阵和当前节点电压和相角,求解线性方程组,得到修正量。

b.更新变量:根据修正量和当前节点电压和相角,更新节点电压和相角的值。

c.判断收敛:判断修正量是否满足收敛条件,如果满足则结束迭代计算,否则返回步骤a。

牛顿-拉夫逊法的优点是收敛速度快,精度高。

然而,它的缺点是对于方程组的收敛性和初始值的选择要求较高,存在收敛到局部最小值的问题。

为了克服这些问题,可以采用改进的牛顿-拉夫逊法,如增加松弛因子或采用多起点迭代法等。

总之,牛顿-拉夫逊法是一种高效的求解非线性方程组和潮流计算问题的数值方法。

它在电力系统潮流计算中广泛应用,帮助分析和评估电力系统的稳定性和功率传输能力。

随着电力系统的规模和复杂性的增加,牛顿-拉夫逊法的进一步改进和优化仍然是一个研究的热点问题。

基于极坐标的牛顿-拉夫逊法潮流计算毕业设计

基于极坐标的牛顿-拉夫逊法潮流计算毕业设计

毕业设计基于极坐标的牛顿-拉夫逊法潮流计算摘要潮流计算是电力系统最基本的计算功能,其基本思想是根据电力网络上某些节点的已知量求解未知量,潮流计算在电力系统中有着独特的作用。

它不仅能确保电力网络能够正常的运行工作、提供较高质量的电能,还能在以后的电力系统扩建中各种计算提供必要的依据。

计算潮流分布的方法很多,本设计主要用的是基于极坐标的牛顿-拉夫逊法。

根据电力系统网络的基本知识,构建出能代表电力系统系统网络的数学模型,然后用牛顿—拉夫逊法反复计算出各个接点的待求量,直到各个节点的待求量满足电力系统的要求。

我们可以画出计算框图,用MATLAB编写出程序,来代替传统的手算算法。

复杂电力系统是一个包括大量母线、支路的庞大系统。

对这样的系统进行潮流分析时,采用人工计算的方法已经不再适用。

计算机计算已逐渐成为分析复杂系统潮流分布的主要方法。

本设计中还用了一个五节点的电力系统网络来验证本设计在实际运行中的优越性。

关键词:牛顿-拉夫逊法,复杂电力系统,潮流计算The method of Newton- Raphson based on polarABSTRACTPower system load flow calculation is the most basic computing functions, the basic idea is based on some of the electricity network nodes to solve the unknown quantity of known volume,In power system, power flow, which can ensure that electrical net can work well and give the high quality power, but also later provide the necessary datas in the enlargement of the power system. has special function.There are lots of methods about power flow. We mainly use the method ofNewton-Raphson based on polar in my design. According to the basic knowledge of the electrical network, we established the mathematics model which can presents the power system ,then computed again and again unknown members of the each bus with the method of Newton-RaphSon until the unknown numbers meet the demand of the power system. We can write down the block diagram and write the order with the Matlab in place of the traditional methods. Complex power system is a large system which involves lots of bus bars and branches. We also chose a five-bus power system for testing the advantages in the relity.KEY WORDS: Newton-Raphson,power system,power flow目录前言 (1)第一章电力系统潮流计算的基本知识 (2)1.1潮流计算的定义及目的 .............................. 2厦礴恳蹒骈時盡继價骚。

电力系统网络潮流计算—牛顿拉夫逊法

电力系统网络潮流计算—牛顿拉夫逊法

电力系统网络潮流计算—牛顿拉夫逊法牛顿拉弗逊法(Newton-Raphson Method)是一种常用的电力系统网络潮流计算方法,用于求解复杂电力系统中的节点电压和支路潮流分布。

本文将对牛顿拉弗逊法进行详细介绍,并讨论其优缺点及应用范围。

牛顿拉弗逊法的基本原理是通过迭代计算,将电力系统网络潮流计算问题转化为一个非线性方程组的求解问题。

假设电力系统有n个节点,则该方程组的节点电压和支路潮流分布可以通过以下公式表示:f(x)=0其中,f为非线性函数,x为待求解的节点电压和支路潮流分布。

通过泰勒展开,可以将f在其中一点x_k处展开为:f(x)≈f(x_k)+J_k(x-x_k)其中,J_k为f在x_k处的雅可比矩阵,x_k为当前迭代步骤的解。

通过令f(x)≈f(x_k)+J_k(x-x_k)=0,可以求解方程J_k(x-x_k)=-f(x_k),得到下一步的迭代解x_{k+1}。

通过不断迭代,可以逐步接近真实的解,直到满足收敛条件为止。

牛顿拉弗逊法的迭代公式如下:x_{k+1}=x_k-(J_k)^{-1}f(x_k)其中,(J_k)^{-1}为雅可比矩阵J_k的逆矩阵。

牛顿拉弗逊法的优点之一是收敛速度快。

相比其他方法,如高斯赛德尔法,牛顿拉弗逊法通常需要更少的迭代次数才能达到收敛条件。

这是因为牛顿拉弗逊法利用了函数的一阶导数信息,能够更快地找到接近解的方向。

然而,牛顿拉弗逊法也存在一些缺点。

首先,该方法要求求解雅可比矩阵的逆矩阵,计算量较大。

尤其是在大型电力系统网络中,雅可比矩阵往往非常大,计算逆矩阵的复杂度高。

其次,如果初始猜测值不合理,可能会导致算法无法收敛,需要选择合适的初始值,否则可能陷入局部极小值。

牛顿拉弗逊法在电力系统网络潮流计算中有广泛的应用。

该方法可以用于计算节点电压和支路潮流分布,提供电力系统分析和设计的重要数据。

它可以用于稳态分析、短路分析、负荷流分析等多种电力系统问题的求解。

这些问题在电力系统规划、运行和控制等方面都具有重要意义。

基于极坐标的牛顿拉夫逊潮流计算

基于极坐标的牛顿拉夫逊潮流计算

基于极坐标的牛顿拉夫逊潮流计算引言:牛顿-拉夫逊潮流计算是电力系统潮流计算的一种常用方法,用于评估电力系统的电压、功率等参数。

在传统的牛顿-拉夫逊潮流计算中,节点的注入功率和节点电压之间用直角坐标系表示,但在一些情况下,使用直角坐标系并不方便。

因此,基于极坐标的牛顿-拉夫逊潮流计算应运而生。

本文将介绍基于极坐标的牛顿-拉夫逊潮流计算的原理和步骤。

一、基本原理基于极坐标的牛顿-拉夫逊潮流计算使用极坐标系来表示节点的注入功率和节点电压。

在极坐标中,节点的注入功率复数可以表示为S=P+jQ,其中P为有功功率,Q为无功功率。

节点的电压复数可以表示为V=V∠θ,其中V为电压幅值,θ为电压相角。

使用复数的运算规则可以推导出通过变压器、感性和容性元件的电流和功率的计算公式。

二、步骤1.初始化:a.设置节点电压估计值V0和电压相角估计值θ0。

b.将节点注入功率S注入1设置为节点P和Q的初始估计值。

2.计算注入电流:a. 计算节点注入电流I^inj = S^inj / V0^*,其中^*表示复共轭。

b. 计算节点电流注入I^ = I^inj + Σ I^flow,其中Σ表示对所有与节点连接的边的求和,I^flow为边的注入电流,需要通过变压器、感性和容性元件的运算公式计算。

3.更新节点电压:a.计算新的节点电压的幅值和相角:V = ,I^flow, * Zflow,这里Zflow为边的阻抗。

θ = Arg(I^flow) + φflow,φflow为边的阻抗相角。

b.计算新的节点电压估计值V0和电压相角估计值θ0。

V0 = ,I^inj, * Z1 + V * Z2,其中Z1和Z2为接地导线的阻抗。

θ0 = Arg(I^inj) + Arg(V)。

4.更新节点注入功率:a. 计算节点注入功率复数S^inj = P + jQ。

b. 将节点注入功率复数S^inj转化为直角坐标系中的实部和虚部,得到新的节点有功功率和无功功率。

外文翻译--基于优化的牛顿—拉夫逊法和牛顿法的潮流计算

外文翻译--基于优化的牛顿—拉夫逊法和牛顿法的潮流计算

外文翻译--基于优化的牛顿—拉夫逊法和牛顿法的潮流计算英文文献Power Flow Calculation by Combination of Newton-Raphson Method and Newton’s Method in Optimization.Andrey Pazderin, Sergey YuferevURAL STATE TECHNICAL UNIVERSITY ? UPIE-mail: pav@//0>., usv@//.Abstract--In this paper, the application of the Newton’s method in optimization for power flow calculation is considered. Convergence conditions of the suggested method using an example of a three-machine system are investigated. It is shown, that the method allows to calculate non-existent state points and automatically pulls them onto the boundary of power flow existence domain. A combined method which is composed of Newton-Raphson method and Newton’s method in optimization is presented in the paper.Index Terms?Newton method, Hessian matrix, convergence of numerical methods, steady state stabilityⅠ.INTRODUCTIONThe solution of the power flow problem is the basis on which otherproblems of managing the operation and development of electrical power systems EPS are solved. The complexity of the problem of power flow calculation is attributed to nonlinearity of steady-state equations system and its high dimensionality, which involves iterative methods. The basic problem of the power flow calculation is that of the solution feasibility and iterative process convergence [1].The desire to find a solution which would be on the boundary of the existence domain when the given nodal capacities are outside the existence domain of the solution, and it is required to pull the state point back onto the feasibility boundary, motivates to develop methods and algorithms for power flow calculation, providing reliable convergence to the solution.The algorithm for the power flow calculation based on the Newton's method in optimization allows to find a solution for the situation when initial data are outside the existence domain and to pull the operation point onto the feasibility boundary by an optimal path. Also it is possible to estimate a static stability margin by utilizing Newton's method in optimization.As the algorithm based on the Newton’s method in optimization has considerable computational cost and power control cannot be realized in all nodes, the algorithm based on the combination of the Newton-Raphson met hods and the Newton’s method in optimization is offered to be utilizedfor calculating speed, enhancing the power flow calculation.II. THEORETICAL BACKGROUNDA.Steady-state equationsThe system of steady-state equations, in general, can be expressed as follows: where is the vector of parameters given for power flow calculation. In power flow calculation, real and reactive powers are set in each bus except for the slack bus. Ingeneration buses, the modulus of voltage can be fixed. WX,Y is the nonlinear vector function of steady-state equations. Variables Y define the quasi-constant parameters associated with an equivalent circuit of an electrical network. X is a required state vector, it defines steady state of EPS. The dimension of the state vector coincides with the number of nonlinear equations of the system 1. There are various known forms of notation of the steady-state equations. Normally, they are nodal-voltage equations in the form of power balance or in the form of current balance. Complex quantities in these equations can be presented in polar or rectangular coordinates, which leads to a sufficiently large variety forms of the steady-state equations notation. There are variable methods of a nonlinear system of steady-state equations solution. They are united by the incremental vector of independent variables ΔX being searched and the condition of convergence being assessed at each iteration.B. The Newton's method in optimizationAnother way of solving the problem of power flow calculation is related to defining a zero minimum of objective function of squares sum of discrepancies of steady-stateequations:2?The function minimum 2 is reached at the point where derivatives on all required variables are equal to zero: 3It is necessary to solve a nonlinear set of equations 3 to find the solution for the problem. Calculating the power flow, which is made by the system of the linear equations with a Hessian matrix at each iteration, is referred to as the Newton'smethod in optimization [4]: 4The Hessian matrix contains two items: 5During the power flow calculation, the determinant of Hessian matrix is positive round zero and negative value of a determinant of Jacobian .This allows to find the state point during the power flow calculation, when initial point has been outside of the existence domain.The convergence domain of the solution of the Newton's optimization method is limited by a positive value of the Hessian matrix determinant. The iterative process even for a solvable operating point can converge to an incorrectsolution if initial approximation has been outside convergencedomain. This allows to estimate a static stability margin of the state and to find the most perilous path of its weighting.III. INVESTIGATIONS ON THE TEST SCHEMEConvergence of the Newton's method in optimization with a full Hessian matrix has been investigated. Calculations were made based on program MathCAD for a network comprising three buses the parameters of which are presented in Figure 1.Dependant variables were angles of vectors of bus voltage 1 and 2 ,independent variables were capacities in nodes 1 and 2, and absolute values of voltages of nodes 1, 2 and 3 were fixed.Fig. 1 ? The Test schemeIn Figure 2, the boundary of existence domain for a solution of the steady-state is presented in angular coordinates δ1-δ2. This boundary conforms to a positive value of the Jacobian determinant:As a result of the power flow calculation based on the Newton method in optimization, the angle values have been received, these values corresponding to the given capacities in Fig.2 generation is positive and loading is negative.For the state points which are inside the existence domain, the objective function 2 has been reduced to zero. For the state points which are on the boundary of the existence domain, objective function 2 has not been reduced to zero and the calculated values of capacities differed fromthe given capacities.Fig. 2 ? Domain of Existence for a SolutionFig.3 - Boundary of existence domain In Fig.3, the boundary of the existence domain is presented in coordinates of capacities P1-P2. State points occurring on the boundary of the existence domain 6 have been set by the capacities which were outside the existence domain. As a result of power flow calculation by minimization 2 based on the Newton's method in optimization, the iterative process converges to the nearest boundary point. It is due to the fact that surfaces of the equal level of objective function 2 in coordinates of nodal capacities are proper circles for threemachine system having the centre on the point defined by given values of nodal capacitiesThe graphic interpretation of surfaces of the equal level of objective function for operating point state with 13000 MW loading bus 1 and 15000 MW generating bus 2 is presented in Fig.3.Hessian matrix is remarkable in its being not singular on the boundary of existence domain. The determinant of a Hessian matrix 5 is positive around zero and a negative value of the Jacobian matrix determinant. This fact allows the power flow to be calculated even for the unstable points which are outside existence domain. The iterative process based on the system of the linear equations 4 solution has converged to the critical stability point within 3-5 iteration. Naturally,the iterative process based on Newton-Rapson method is divergent for such unsolvable operating points.The convergence domain of the method under consideration has been investigated. What is meant is that not all unsolvable operating points will be pulled onto theboundary of existence domain. A certain threshold having been exceeded the iterative process has begun to converge to the imaginary solution with angles exceeding 360It is necessary to note that to receive a critical stability operating point in case when initial nodal capacities are set outside the boundary of the existence domain, there is no necessity to make any additional terms as the iterative process converges naturally to the nearest boundary point.Pulling the operation point onto feasibility boundary is not always possible by the shortest and optimal path. There are a number of constraints, such as impossibility of load consumption increase at buses, constraints of generation shedding/gaining at stations. Load following capability of generator units is various, consequently for faster pulling the operation point onto the feasibility boundary it is necessary to carry out this pulling probably by longer, but faster path.The algorithm provides possibility of path correction of pulling. It is carried out by using of the weighting coefficients, which define degree of participation of eachnode in total control action. For this purpose diagonal matrix A of the weighting coefficients for each node is included into the objective function 2:All diagonal elements of the weighting coefficient matrix A should be greater-than zero:When initial approximation lies into the feasibility domain, coefficients are not influence on the computational process and on the result.In the figure 4 different paths of the pulling the same operation point onto feasibility boundary depending on the weighting coefficients are presented. Paths are presented for two different operating points.In tables I and II effect of weighting coefficients on the output computation is presented. In tables I and II k1 and k2 are weighting coefficient for buses 1 and 2, respectively.TABLE IWEIGHTING COEFFICIENT EFFECT ON OUTPUT COMPUTATION FOR INITIAL SET CAPACITIES P1 -13000 MW AND P2 15000 MWCoefficients ,MW ,MW ,deg ,deg1,1 -7800 9410 -45 555,1 -8600 8080 -69 250.005,1 -5700 10140 -1 93TABLE IIWEIGHTING COEFFICIENT EFFECT ON OUTPUT COMPUTATION FOR INITIAL SET CAPACITIES P1 -8000 MW AND P2 -5000 MWCoefficients ,MW ,MW ,deg ,deg1,1 -4360 -1680 -92 -800.01,1 -1050 -4920 -76 -941,0.35 5800 0 -99 -71Fig.4 - Paths of pulling the operation point onto the feasibility boundaryIV. COMBINATION OF METHODSIf to compare the Newton’s method in optimization for power flow calculation with newton-Raphson using a Jacobian matrix, the method computational costs on eachiteration will be several times greater as the property of Hessian matrix being filled up by nonzero elements 2.5-3 times greater than with Jacobian one. Each row of Jacobian matrix corresponding to any bus contains nonzero elements corresponding to all incident buses of the scheme. Each row of Hessian matrix contains nonzero elements in the matrix corresponding not only to the neighboring buses, but also their neighbors. However, it is possible to compensate this disadvantage through the combination Newton-Rap son method with Newton’s method in optimization. It means that the part of nodes can be calculated by conventional Newtonmethod, and the remaining buses will be computed by Newton’s method in optimization. The first group of passive nodes consists of buses in which it is not possible to changenodal capacity or it is not expedient. Hence, emergency control actions are possible only in a small group of buses supplying with telecontrol. Most of the nodes includingpurely transit buses are passive. Active nodes are generating buses in which operating actions are provided. Such approach allows to fix nodal capacity for all passive buses of the scheme which have been calculated by Newton-Rap son method. In active buses which have been calculated by Newton’s method in optimization, deviations from set values of nodal capacity are possible. These deviations can be considered as control action. The power flow calculation algorithm based on combination Newton ? Ra phson method and Newton’s method in optimization can be presented as follows:1.The linear equation system with Jacobian matrix is generated for all buses of the scheme.2. The solution process of the linear equation system with Jacobian is started by utilizing the Gauss method for all passive buses. Factorization of the linear equations system is terminated when all passive buses are eliminated. Factorizedequations are kept.3.The nodal admittance matrix is generated from not factorized the part of Jacobian matrix corresponding to active buses. This admittance matrix contains parameters of the equivalent network which contains only active buses.4.The linear equation system with Hessian matrix 4 is generated for the obtained equivalent by Newton’s method in optimization.5.The linear equation system with Hessian matrix is calculated and changes of independent variables are defined for active buses.6.Factorized equations of passive buses are calculated, and changes of independent variables are defined for passive buses.7.The vector of independent variables is updated using the changes of independent variables for all buses.8. New nodal capacities in all buses of the network are defined; constraints are checked; if it necessary, the list of active buses will be corrected.9. Convergence of the iterative process is checked. If changes of variables are significant, it is necessary to return to item 1.Taking into account the number of active buses in the network aren’t large, computationa l costs of such algorithm slightly exceed computational costs of the Newton-Rapson method.V. CONCLUSION1. The power flow calculation of an electric network by minimizingthe square sum of discrepancies of nodal capacities based on the Newton's method in optimizationmaterially increases the productivity of deriving a solution for heavy in terms of conditions of stability states and the unstable states outside the existence domain of the solution.2. During the power flow calculation, the determinant of Hessian matrix is positive around zero and negative value of the Jacobian matrix determinant. The iterative process naturally converges to the nearest marginal state point during the power flow calculation, when the initial operating point has been outside of the existence domain.3. There is a possibility of control action correction for the pulling operation point onto feasibility boundary by using matrix of weighting coefficients.4. Utilization of the combined method for power flow calculation all ows to use all advantages of Newton’s method in optimization and to provide high calculating speed.5. In case when the setting nodal powers are outside the existence domain, there are discrepancies in the active buses, which can be considered as control actions for pulling the state point onto the feasibility boundary. When the initial state point is inside the existence domain, the iterative process converges with zero discrepancies for both active and passive buses.中文翻译基于优化的牛顿??拉夫逊法和牛顿法的潮流计算摘要??在本文中,考虑到了优化的牛顿法在潮流计算中的应用。

简化牛顿—拉夫逊法在电网潮流计算中的应用

简化牛顿—拉夫逊法在电网潮流计算中的应用

简化牛顿—拉夫逊法在电网潮流计算中的应用【摘要】电网潮流计算需要复杂的计算,工作量较大。

本文改进了牛顿-拉夫逊潮流算法中修正方程式的建立,继而对直角坐标下牛顿-拉夫逊潮流算法的雅可比矩阵进行简化。

26节点算例计算结果表明,该法具有良好的收敛性,减少内存占有量并具有较高的计算速度。

【关键词】潮流计算;牛顿-拉夫逊算法;简化;最优乘子1.引言电力系统潮流计算使用的数学模型是一组多元非线性方程组,直接求解是十分困难甚至是不可能的。

牛顿-拉夫逊法(简称牛顿法)在数学上是求解非线性代数方程式的有效方法。

现代电力系统潮流计算最常用的方法就是牛顿-拉夫逊法。

本文讨论的方法是直角坐标下牛顿-拉夫逊潮流算法的一种简化。

2.牛顿-拉夫逊算法的缺陷牛顿-拉夫逊法是电力系统潮流计算的基本方法,它有收敛快、精度高等特点。

其不足之处有:(1)雅可比矩阵J是一个2(n-1)×2(n-1)的方阵,所以当系统节点很多时,会占用很多的存储单元,虽然用稀疏技术后有所改观,但是采用稀疏技术后在编程时将会降低程序的可读性,增加效验程序的难度;(2)每一次迭代过程中都要分别计算雅可比矩阵J中每一个非零元素,使得每一次迭代的计算量都很大;(3)由于一般电力系统中J的阶数较高,也会相应增加求解的计算量。

鉴于牛顿-拉夫逊法的上述特点,在下文中将对其简化得出一种改进的牛顿潮流计算的解法。

3.牛顿-拉夫逊算法的改进3.1 雅可比矩阵J的简化在高压电力系统中,由于,所以可以近似认为,于是:因此,在电力系统运行中,其有功功率的不平衡量主要由电压的相位变化引起,而电压的幅值主要影响无功功率的不平衡量,即可以近似认为的变化只引起电压虚部、的变化,的变化只引起电压实部、的变化,的变化只引起、的变化。

因此,雅可比矩阵元素中,,。

所以矩阵可改为:在交流高压电网中,输电线路的电抗要比电阻大得多,即:。

而电导:故电力系统在实际运行中,系统参数。

在一般情况下,线路两端电压的相角差是不大的(通常不超过10o~20o),所以在初次迭代时电压的虚部可近似为零。

基于牛顿拉夫逊法的电力系统潮流计算毕业设计(论文) 精品

基于牛顿拉夫逊法的电力系统潮流计算毕业设计(论文) 精品
60年代初期,数字计算机已发展到第二代,计算机的内存和速度发生了很大的飞跃,从而为阻抗法的采用创造了条件。阻抗法要求数字计算机贮存表征系统接线和参数的阻抗矩阵,这就需要大量的内存。而且阻抗法每迭代一次都要求顺次取阻抗矩阵中的每一个元素进行计算,因此,每次迭代的运算量很大。这两种情况都是过去电子管计算机无法适应的。
在电网的设计规划阶段,通过潮流计算,合理的规划接入电源的容量和接入点,合理规划电网的结构,选择无功补偿方案,满足规划水平的大、小方式下的交流交换控制、调峰、调相、调压的要求 。
在编年制运行方式时,在预计负荷增长及新设备投运基础上进行潮流计算,可以预计电网的运行情况,发现电网中的薄弱环节,供调度员日常调度控制参考,并为电网改造提供建议和依据 。
一、
在电力系统规划设计和现有的电力系统的运行方式的研究中,都需要用潮流计算来定量的分析比较供电方案或运行方式的合理性、可靠性和经济性。此外,电力系统潮流计算也是计算系统动态稳定和静态稳定的基础。所以潮流计算是电力系统一种最重要最基本的运算 。
电力系统的潮流计算也分为离线计算和在线计算两种,前者主要用于系统的规划设计和安排系统的运行方式,后者则用于正在运行系统的实时监视和控制。
TheNewton- Raphson power flow calculationhasa relatively high demand for a given initial value. SobeforetheNewton- Raphson iteration, weuseGauss - Seidel iterative methodtoproduce a more precise initial value. This paper describes theprocessofGauss - Seidel andNewton- Raphson iteration. The main contentsarethe establishment of iterative equation, the calculation of Jacobian matrixandthe calculation of power and voltage, as well ashow to deal with thesituationwhen aPV nodetransform toa PQ node iterationprocess.We use theMatlab programming languageas development tools,the input and output of the data process in theExcel spreadsheets.

基于极坐标的牛顿拉夫逊法潮流计算设计

基于极坐标的牛顿拉夫逊法潮流计算设计

基于极坐标的牛顿拉夫逊法潮流计算设计极坐标是一种非常有效的数学工具,可用于描述圆形或球形的物体。

在潮流计算中,借助极坐标可以更准确地描述电网中节点之间的电流和电压。

牛顿拉夫逊法(Newton-Raphson method)是一种数值计算方法,用于求解非线性方程组。

在潮流计算中,我们需要求解电网中节点的电压相位和模值,这可以通过牛顿拉夫逊法进行迭代计算。

潮流计算的目标是确定电网中各个节点的电压相位和模值,以及支路中的电流大小和相位差。

利用极坐标可以更直观地表示电流和电压的相位差。

在设计基于极坐标的牛顿拉夫逊法潮流计算时,首先需要建立电网的节点导纳矩阵和负荷模型。

然后,可以开始迭代计算,以下是该方法的步骤:1.初始化节点电压的相位和模值。

可以使用已知的节点电压作为初始猜测值。

2.计算节点注入功率,包括负荷注入功率和支路注入功率。

3.计算节点电流注入向量,通过求解节点电压和节点注入功率之间的关系。

4.根据电流注入向量,计算雅可比矩阵。

雅可比矩阵描述了节点电流注入向量与节点电压之间的关系。

5.利用雅可比矩阵和节点电流注入向量,求解节点电压的变化量。

可以使用牛顿迭代公式进行计算。

6.更新节点电压,计算新的节点电压值。

7.判断节点电压是否收敛。

如果未收敛,返回步骤4进行下一次迭代;如果已收敛,结束迭代过程。

通过以上迭代计算,可以求得电网中各个节点的电压相位和模值。

基于极坐标的计算结果可以更清晰地展示节点之间的电流和电压关系,有助于对电网的运行状态进行分析和优化。

综上所述,基于极坐标的牛顿拉夫逊法潮流计算设计十分可行和有效。

该方法能够提供更准确的节点电压和电流信息,有助于电力系统的运行控制和优化。

基于极坐标的牛顿拉夫逊法潮流计算设计

基于极坐标的牛顿拉夫逊法潮流计算设计

基于极坐标的牛顿拉夫逊法潮流计算设计极坐标的牛顿拉夫逊法潮流计算是一种在电力系统分析中广泛使用的方法。

它通过使用极坐标来表示节点电压和角度,对电力系统的潮流进行计算。

这种方法具有计算速度快、收敛性好等优点,在实际工程中具有很高的实用性。

首先,我们需要明确定义该计算的目标。

潮流计算的目标是计算电力系统中各个节点的电压幅值和相角,以及系统中每一根支路上的潮流大小和方向。

这些计算结果可以帮助我们了解电力系统中的潮流分布情况,并为系统的运行与调度提供指导。

极坐标的牛顿拉夫逊法潮流计算的核心思想是通过迭代计算节点的电压幅值和相角,最终使得系统总功率平衡和节点潮流满足潮流方程。

这个方法的基本步骤可以总结为以下几步:1.初始化电压幅值和相角:首先,我们需要对电力系统中各个节点的电压幅值和相角进行初始化。

这可以通过读取系统的初始状态或者通过简化的方法进行估算得到。

2.计算节点注入功率:根据节点电压和相角,以及负载和发电机的参数,计算每个节点的注入功率(即电流乘以电压的复数形式)。

这个计算可以使用潮流方程进行表达。

3.计算雅可比矩阵:根据节点注入功率的变化对节点电压的变化进行线性近似,得到雅可比矩阵。

雅可比矩阵的元素可以通过潮流方程的偏导数计算得到。

4.解线性方程:通过雅可比矩阵和节点注入功率的计算结果,求解线性方程组。

这个方程组的解表示节点电压的变化量。

5.更新节点电压:根据线性方程组的解,更新节点的电压幅值和相角。

6.检查收敛准则:判断节点电压的更新是否符合收敛准则。

如果不满足准则,返回步骤4;如果满足准则,继续下一步。

7.计算支路潮流:根据节点电压幅值和相角,以及支路的参数,计算每一根支路上的潮流大小和方向。

这个计算可以使用潮流方程进行表达。

8.检查潮流误差:判断计算得到的支路潮流是否与预期的值相符合。

如果不符合,则调整节点电压,并返回步骤4;如果符合,则计算结束。

上述步骤中的潮流方程可以根据电力系统的拓扑结构和支路参数,以及节点电压和功率注入的情况,进行建模和推导。

在配电网中基于牛顿-拉夫逊法解最优潮流的应用

在配电网中基于牛顿-拉夫逊法解最优潮流的应用

在配电网中基于牛顿-拉夫逊法解最优潮流的应用赵君;于泓;赵华松【摘要】Power flow calculation is an important solution of determining the basic data of electric system. Optimal power flow is the condition of maintaining low cost for the entire power system. The article expounds how to achieve the minimum value of cost function by adjusting the output of generators on the basis of Newton-Laphson. It has significant meaning for judging the optimum operation and development of present system.%潮流计算是用来确定电力系统基本数据的重要解决方案,最优潮流是整个电力系统成本最低的条件。

基于牛顿—拉夫逊法,通过调节发电机的输出口来实现成本函数的最小值,对于判定现有系统的最佳运行和发展具有重要意义。

【期刊名称】《农业科技与装备》【年(卷),期】2014(000)010【总页数】3页(P34-36)【关键词】电力系统;潮流计算;牛顿-拉夫逊法;最优潮流;目标函数【作者】赵君;于泓;赵华松【作者单位】沈阳农业大学信息与电气工程学院,沈阳 110866;沈阳农业大学信息与电气工程学院,沈阳 110866;沈阳农业大学信息与电气工程学院,沈阳110866【正文语种】中文【中图分类】TP273电力系统潮流中的牛顿—拉夫逊法首次应用于20世纪60年代,该方法解决了早期阿尔瓦拉多和托马斯研究方法的收敛性较差的问题。

牛顿拉夫逊法潮流计算

牛顿拉夫逊法潮流计算

牛顿拉夫逊法潮流计算摘要本文,首先简单介绍了基于在MALAB中行潮流计算的原理、意义,然后用具体的实例,简单介绍了如何利用MALAB去进行电力系统中的潮流计算。

众所周知,电力系统潮流计算是研究电力系统稳态运行情况的一种计算,它根据给定的运行条件及系统接线情况确定整个电力系统各部分的运行状态:各线的电压、各元件中流过的功率、系统的功率损耗等等。

在电力系统规划的设计和现有电力系统运行方式的研究中,都需要利用潮流计算来定量地分析比较供电方案或运行方式的合理性、可靠性和经济性。

此外,在进行电力系统静态及暂态稳定计算时,要利用潮流计算的结果作为其计算的基础;一些故障分析以及优化计算也需要有相应的潮流计算作配合;潮流计算往往成为上述计算程序的一个重要组成部分。

以上这些,主要是在系统规划设计及运行方式安排中的应用,属于离线计算范畴。

牛顿-拉夫逊法在电力系统潮流计算的常用算法之一,它收敛性好,迭代次数少。

本文介绍了电力系统潮流计算机辅助分析的基本知识及潮流计算牛顿-拉夫逊法,最后介绍了利用MTALAB程序运行的结果。

关键词:电力系统潮流计算,牛顿-拉夫逊法,MATLABABSTRACTThis article first introduces the flow calculation based on the principle of MALAB Bank of China, meaning, and then use specific examples, a brief introduction, how to use MALAB to the flow calculation in power systems.As we all know, is the study of power flow calculation of power system steady-state operation of a calculation, which according to the given operating conditions and system wiring the entire power system to determine the operational status of each part: the bus voltage flowing through the components power, system power loss and so on. In power system planning power system design and operation mode of the current study, are required to quantitatively calculated using the trend analysis and comparison of the program or run mode power supply reasonable, reliability and economy.In addition, during the power system static and transient stability calculation, the results of calculation to take advantage of the trend as its basis of calculation; number of fault analysis and optimization also requires a corresponding flow calculation for cooperation; power flow calculation program often become the an important part. These, mainly in the way of system design and operationarrangements in the application areas are off-line calculation.Newton - Raphson power flow calculation in power system is one commonly used method, it is good convergence of the iteration number of small, introduce the trend of computer-aided power system analysis of the basic knowledge and power flow Newton - Raphson method, introduced by the last matlab run results.Keywords:power system flow calculation, Newton – Raphson method, matlab目录1 绪论 (1)1.1 课题背景 (1)1.2 电力系统潮流计算的意义 (2)1.3 电力系统潮流计算的发展 (2)1.4 潮流计算的发展趋势 (4)2 潮流计算的数学模型 (5)2.1 电力线路的数学模型及其应用 (5)2.2 等值双绕组变压器模型及其应用 (6)2.3 电力网络的数学模型 (9)2.4 节点导纳矩阵 (10)2.4.1 节点导纳矩阵的形成 (10)2.4.2 节点导纳矩阵的修改 (11)2.5 潮流计算节点的类型 (12)2.6 节点功率方程 (12)2·7 潮流计算的约束条件 (14)3 牛顿-拉夫逊法潮流计算基本原理 (15)3.1 牛顿-拉夫逊法的基本原理 (15)3.2 牛顿-拉夫逊法潮流计算的修正方程 (18)3.3 潮流计算的基本特点 (21)3.4 节点功率方程 (22)4牛顿-拉夫逊法分解潮流程序 (23)4·1 牛顿-拉夫逊法分解潮流程序原理总框图 (23)4.2 形成节点导纳矩阵程序框图及代码 (25)4.2。

牛顿拉夫逊法计算潮流步骤

牛顿拉夫逊法计算潮流步骤

牛顿拉夫逊法计算潮流步骤牛顿拉夫逊法(Newton-Raphson Method)是一种常用于计算潮流的数值求解方法。

它是基于潮流计算的功率流方程的非线性特性而设计的,通过迭代求解来逼近潮流计算的稳态解。

下面将介绍牛顿拉夫逊法计算潮流的基本步骤。

首先,我们需要明确潮流计算的目标,即确定电力系统中各节点的电压相角和幅值。

这些节点是电力系统中的发电机、负荷和交流输电线路的连接点。

通过潮流计算,我们可以得到各节点的电压相角和幅值,从而分析系统的功率分布、电压稳定性等运行特性。

接下来,我们需要建立电力系统的潮流计算模型。

这个模型中,我们需要考虑发电机的注入功率、负荷的吸收功率、线路的传输损耗等因素。

通过利用功率流方程,我们可以将这些因素表示为电压、功率和导纳之间的方程。

然后,我们需要进行初始化操作。

在进行牛顿拉夫逊法迭代计算之前,我们需要对电力系统的各节点进行初始电压值的设定。

这些初始值可以根据经验或者历史数据来得到,但需要满足物理约束条件,如一致性、电压幅值在合理范围内等。

接下来,我们进入迭代计算的过程。

首先,我们需要对系统的节点进行编号,然后选择某一节点作为基准节点,其他节点相对于基准节点的电压相角进行计算。

然后,我们根据节点注入功率和导纳矩阵的关系,得到节点注入电流。

接着,我们根据节点注入电流和电压相角的关系,计算各节点的电压相角和幅值的改变量。

在计算改变量后,我们需要对节点电压进行更新。

更新后,我们判断系统是否达到收敛条件。

如果满足收敛条件,则停止迭代,得到最终的潮流计算结果;如果不满足收敛条件,则继续进行下一轮迭代计算。

最后,我们对潮流计算结果进行分析和验证。

通过比较计算得到的结果和实际运行数据进行对比,我们可以评估潮流计算的准确性。

同时,我们还可以通过故障分析、电压稳定性评估等手段对电力系统进行优化和改进。

总而言之,牛顿拉夫逊法是一种常用的求解潮流计算问题的方法。

它通过迭代求解潮流计算的功率流方程,逼近潮流计算的稳态解。

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外文翻译--基于优化的牛顿—拉夫逊法和牛顿法的潮流计算英文文献Power Flow Calculation by Combination of Newton-Raphson Method and Newton’s Method in Optimization.Andrey Pazderin, Sergey YuferevURAL STATE TECHNICAL UNIVERSITY ? UPIE-mail: pav@//0>., usv@//.Abstract--In this paper, the application of the Newton’s method in optimization for power flow calculation is considered. Convergence conditions of the suggested method using an example of a three-machine system are investigated. It is shown, that the method allows to calculate non-existent state points and automatically pulls them onto the boundary of power flow existence domain. A combined method which is composed of Newton-Raphson method and Newton’s method in optimization is presented in the paper.Index Terms?Newton method, Hessian matrix, convergence of numerical methods, steady state stabilityⅠ.INTRODUCTIONThe solution of the power flow problem is the basis on which otherproblems of managing the operation and development of electrical power systems EPS are solved. The complexity of the problem of power flow calculation is attributed to nonlinearity of steady-state equations system and its high dimensionality, which involves iterative methods. The basic problem of the power flow calculation is that of the solution feasibility and iterative process convergence [1].The desire to find a solution which would be on the boundary of the existence domain when the given nodal capacities are outside the existence domain of the solution, and it is required to pull the state point back onto the feasibility boundary, motivates to develop methods and algorithms for power flow calculation, providing reliable convergence to the solution.The algorithm for the power flow calculation based on the Newton's method in optimization allows to find a solution for the situation when initial data are outside the existence domain and to pull the operation point onto the feasibility boundary by an optimal path. Also it is possible to estimate a static stability margin by utilizing Newton's method in optimization.As the algorithm based on the Newton’s method in optimization has considerable computational cost and power control cannot be realized in all nodes, the algorithm based on the combination of the Newton-Raphson met hods and the Newton’s method in optimization is offered to be utilizedfor calculating speed, enhancing the power flow calculation.II. THEORETICAL BACKGROUNDA.Steady-state equationsThe system of steady-state equations, in general, can be expressed as follows: where is the vector of parameters given for power flow calculation. In power flow calculation, real and reactive powers are set in each bus except for the slack bus. Ingeneration buses, the modulus of voltage can be fixed. WX,Y is the nonlinear vector function of steady-state equations. Variables Y define the quasi-constant parameters associated with an equivalent circuit of an electrical network. X is a required state vector, it defines steady state of EPS. The dimension of the state vector coincides with the number of nonlinear equations of the system 1. There are various known forms of notation of the steady-state equations. Normally, they are nodal-voltage equations in the form of power balance or in the form of current balance. Complex quantities in these equations can be presented in polar or rectangular coordinates, which leads to a sufficiently large variety forms of the steady-state equations notation. There are variable methods of a nonlinear system of steady-state equations solution. They are united by the incremental vector of independent variables ΔX being searched and the condition of convergence being assessed at each iteration.B. The Newton's method in optimizationAnother way of solving the problem of power flow calculation is related to defining a zero minimum of objective function of squares sum of discrepancies of steady-stateequations:2?The function minimum 2 is reached at the point where derivatives on all required variables are equal to zero: 3It is necessary to solve a nonlinear set of equations 3 to find the solution for the problem. Calculating the power flow, which is made by the system of the linear equations with a Hessian matrix at each iteration, is referred to as the Newton'smethod in optimization [4]: 4The Hessian matrix contains two items: 5During the power flow calculation, the determinant of Hessian matrix is positive round zero and negative value of a determinant of Jacobian .This allows to find the state point during the power flow calculation, when initial point has been outside of the existence domain.The convergence domain of the solution of the Newton's optimization method is limited by a positive value of the Hessian matrix determinant. The iterative process even for a solvable operating point can converge to an incorrectsolution if initial approximation has been outside convergencedomain. This allows to estimate a static stability margin of the state and to find the most perilous path of its weighting.III. INVESTIGATIONS ON THE TEST SCHEMEConvergence of the Newton's method in optimization with a full Hessian matrix has been investigated. Calculations were made based on program MathCAD for a network comprising three buses the parameters of which are presented in Figure 1.Dependant variables were angles of vectors of bus voltage 1 and 2 ,independent variables were capacities in nodes 1 and 2, and absolute values of voltages of nodes 1, 2 and 3 were fixed.Fig. 1 ? The Test schemeIn Figure 2, the boundary of existence domain for a solution of the steady-sta te is presented in angular coordinates δ1-δ2. This boundary conforms to a positive value of the Jacobian determinant:As a result of the power flow calculation based on the Newton method in optimization, the angle values have been received, these values corresponding to the given capacities in Fig.2 generation is positive and loading is negative.For the state points which are inside the existence domain, the objective function 2 has been reduced to zero. For the state points which are on the boundary of the existence domain, objective function 2 has not been reduced to zero and the calculated values of capacities differed fromthe given capacities.Fig. 2 ? Domain of Existence for a SolutionFig.3 - Boundary of existence domain In Fig.3, the boundary of the existence domain is presented in coordinates of capacities P1-P2. State points occurring on the boundary of the existence domain 6 have been set by the capacities which were outside the existence domain. As a result of power flow calculation by minimization 2 based on the Newton's method in optimization, the iterative process converges to the nearest boundary point. It is due to the fact that surfaces of the equal level of objective function 2 in coordinates of nodal capacities are proper circles for threemachine system having the centre on the point defined by given values of nodal capacitiesThe graphic interpretation of surfaces of the equal level of objective function for operating point state with 13000 MW loading bus 1 and 15000 MW generating bus 2 is presented in Fig.3.Hessian matrix is remarkable in its being not singular on the boundary of existence domain. The determinant of a Hessian matrix 5 is positive around zero and a negative value of the Jacobian matrix determinant. This fact allows the power flow to be calculated even for the unstable points which are outside existence domain. The iterative process based on the system of the linear equations 4 solution has converged to the critical stability point within 3-5 iteration. Naturally,the iterative process based on Newton-Rapson method is divergent for such unsolvable operating points.The convergence domain of the method under consideration has been investigated. What is meant is that not all unsolvable operating points will be pulled onto theboundary of existence domain. A certain threshold having been exceeded the iterative process has begun to converge to the imaginary solution with angles exceeding 360It is necessary to note that to receive a critical stability operating point in case when initial nodal capacities are set outside the boundary of the existence domain, there is no necessity to make any additional terms as the iterative process converges naturally to the nearest boundary point.Pulling the operation point onto feasibility boundary is not always possible by the shortest and optimal path. There are a number of constraints, such as impossibility of load consumption increase at buses, constraints of generation shedding/gaining at stations. Load following capability of generator units is various, consequently for faster pulling the operation point onto the feasibility boundary it is necessary to carry out this pulling probably by longer, but faster path.The algorithm provides possibility of path correction of pulling. It is carried out by using of the weighting coefficients, which define degree of participation of eachnode in total control action. For this purpose diagonal matrix A of the weighting coefficients for each node is included into the objective function 2:All diagonal elements of the weighting coefficient matrix A should be greater-than zero:When initial approximation lies into the feasibility domain, coefficients are not influence on the computational process and on the result.In the figure 4 different paths of the pulling the same operation point onto feasibility boundary depending on the weighting coefficients are presented. Paths are presented for two different operating points.In tables I and II effect of weighting coefficients on the output computation is presented. In tables I and II k1 and k2 are weighting coefficient for buses 1 and 2, respectively.TABLE IWEIGHTING COEFFICIENT EFFECT ON OUTPUT COMPUTATION FOR INITIAL SET CAPACITIES P1 -13000 MW AND P2 15000 MWCoefficients ,MW ,MW ,deg ,deg1,1 -7800 9410 -45 555,1 -8600 8080 -69 250.005,1 -5700 10140 -1 93TABLE IIWEIGHTING COEFFICIENT EFFECT ON OUTPUT COMPUTATION FOR INITIAL SET CAPACITIES P1 -8000 MW AND P2 -5000 MWCoefficients ,MW ,MW ,deg ,deg1,1 -4360 -1680 -92 -800.01,1 -1050 -4920 -76 -941,0.35 5800 0 -99 -71Fig.4 - Paths of pulling the operation point onto the feasibility boundaryIV. COMBINATION OF METHODSIf to compare the Newton’s method in optimization for power flow calculation with newton-Raphson using a Jacobian matrix, the method computational costs on eachiteration will be several times greater as the property of Hessian matrix being filled up by nonzero elements 2.5-3 times greater than with Jacobian one. Each row of Jacobian matrix corresponding to any bus contains nonzero elements corresponding to all incident buses of the scheme. Each row of Hessian matrix contains nonzero elements in the matrix corresponding not only to the neighboring buses, but also their neighbors. However, it is possible to compensate this disadvantage through the combination Newton-Rap son method with Newton’s method in optimization. It means that the part of nodes can be calculated by conventional Newtonmethod, and the remaining buses will be computed by Newton’s method in optimization. The first group of passive nodes consists of buses in which it is not possible to changenodal capacity or it is not expedient. Hence, emergency control actions are possible only in a small group of buses supplying with telecontrol. Most of the nodes includingpurely transit buses are passive. Active nodes are generating buses in which operating actions are provided. Such approach allows to fix nodal capacity for all passive buses of the scheme which have been calculated by Newton-Rap son method. In active buses which have been calculated by Newton’s method in optimization, deviations from set values of nodal capacity are possible. These deviations can be considered as control action. The power flow calculation algorithm based on combination Newton ? Ra phson method and Newton’s method in optimization can be presented as follows:1.The linear equation system with Jacobian matrix is generated for all buses of the scheme.2. The solution process of the linear equation system with Jacobian is started by utilizing the Gauss method for all passive buses. Factorization of the linear equations system is terminated when all passive buses are eliminated. Factorizedequations are kept.3.The nodal admittance matrix is generated from not factorized the part of Jacobian matrix corresponding to active buses. This admittance matrix contains parameters of the equivalent network which contains only active buses.4.The linear equation system with Hessian matrix 4 is generated for the obtained equivalent by Newton’s method in optimization.5.The linear equation system with Hessian matrix is calculated and changes of independent variables are defined for active buses.6.Factorized equations of passive buses are calculated, and changes of independent variables are defined for passive buses.7.The vector of independent variables is updated using the changes of independent variables for all buses.8. New nodal capacities in all buses of the network are defined; constraints are checked; if it necessary, the list of active buses will be corrected.9. Convergence of the iterative process is checked. If changes of variables are significant, it is necessary to return to item 1.Taking into account the number of active buses in the network aren’t large, computationa l costs of such algorithm slightly exceed computational costs of the Newton-Rapson method.V. CONCLUSION1. The power flow calculation of an electric network by minimizingthe square sum of discrepancies of nodal capacities based on the Newton's method in optimizationmaterially increases the productivity of deriving a solution for heavy in terms of conditions of stability states and the unstable states outside the existence domain of the solution.2. During the power flow calculation, the determinant of Hessian matrix is positive around zero and negative value of the Jacobian matrix determinant. The iterative process naturally converges to the nearest marginal state point during the power flow calculation, when the initial operating point has been outside of the existence domain.3. There is a possibility of control action correction for the pulling operation point onto feasibility boundary by using matrix of weighting coefficients.4. Utilization of the combined method for power flow calculation all ows to use all advantages of Newton’s method in optimization and to provide high calculating speed.5. In case when the setting nodal powers are outside the existence domain, there are discrepancies in the active buses, which can be considered as control actions for pulling the state point onto the feasibility boundary. When the initial state point is inside the existence domain, the iterative process converges with zero discrepancies for both active and passive buses.中文翻译基于优化的牛顿??拉夫逊法和牛顿法的潮流计算摘要??在本文中,考虑到了优化的牛顿法在潮流计算中的应用。

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