WO2020088245A1 - 一种基于直算法的电磁机电暂态仿真算法 - Google Patents
一种基于直算法的电磁机电暂态仿真算法 Download PDFInfo
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- the invention belongs to the technical field of electric power system simulation, in particular to an electromagnetic electromechanical transient simulation algorithm based on a straight algorithm.
- the electromechanical transient process and the electromagnetic transient process in the power system are two physical processes that are characterized by different mathematical models and have different time constants. In traditional power system analysis tools, these two processes are usually digitally simulated separately. Compared with electromechanical transient simulation, the mathematical model of power equipment under electromagnetic transient is more complicated, and the dynamic time constant concerned is smaller, which greatly increases the calculation amount and calculation time of simulation, and it is much more difficult to realize real-time digital simulation of a certain scale system. .
- Electromagnetic transient process digital simulation is a numerical simulation method to simulate the electromagnetic transient process in the power system from several microseconds to several seconds.
- the electromagnetic transient process simulation must consider the transmission line distribution parameter characteristics and parameter frequency characteristics, the generator's electromagnetic and electromechanical transient processes and the nonlinear characteristics of a series of components (arrester, transformer, reactor, etc.). Therefore, the mathematical model of electromagnetic transient simulation must establish algebraic or differential and partial differential equations for these components and systems.
- the commonly used numerical integration method is implicit integration.
- electromagnetic transient simulation requires not only a detailed nonlinear model for the dynamic components of the power system, but also the transient process of the network, it also needs to be described by differential equations, which limits the simulation scale of electromagnetic transient simulation programs.
- the power system must be simplified by equivalent.
- the simulation of the electromechanical transient process mainly studies the transient stability of the power system after large disturbances and the static stability performance after small disturbances.
- the transient stability analysis is to study the power system's dynamic behavior and ability to maintain synchronous and stable operation when the power system is subjected to large disturbances such as short circuit faults, removal of lines, generators, and loads, loss of excitation or shock load of the generator.
- the algorithm of electromechanical transient simulation of power system is to solve the system of differential equations and algebraic equations of power system simultaneously to obtain the time domain solution of the physical quantity.
- the methods of solving differential equations mainly include implicit trapezoidal integration method, improved Euler method, Runge-Kutta method, etc. Among them, implicit trapezoidal integration method is getting more and more applications because of its good numerical stability.
- the method of solving algebraic equations mainly uses the Newton method which is suitable for solving nonlinear algebraic equations. According to the order of solving differential equations and algebraic equations, it can be divided into alternating solutions and simultaneous solutions.
- the name of the invention is: a straight chain and branched chain three-phase symmetric multi-power non-loop network power system straight algorithm provides a precise calculation result, fast operation speed three-phase symmetric multi-power Non-loop power flow straight algorithm;
- the application number is CN201610783305.3, and the name of the invention is: a direct calculation method based on the ring network power system.
- This patent mainly solves the error of the calculation result of the iterative method applied by the existing ring network power flow algorithm. Slowness and other issues;
- the application number is CN201810219284.1, and the name of the invention is: a straight algorithm-based electromechanical transient simulation method of power system, which overcomes the defects of the traditional simulation method, without iteration, fast calculation speed, high accuracy and small error, real
- the ground reflects the changing characteristics of the power grid, such as the impedance of each line, load and transformer changes with the frequency of the power grid, and the frequency of each generator in the power grid can also dynamically change according to their own laws;
- the object of the present invention is to provide an electromagnetic electromechanical transient simulation algorithm based on a straight algorithm to achieve a simulation calculation that can realize electromagnetic transient integration.
- the technical scheme adopted by the present invention is: an electromagnetic electromechanical transient simulation algorithm based on a straight algorithm.
- the power system simulation includes a generator model, a line model, a load model, and a transformer model.
- the generator model and the line model are calculated separately.
- the electromagnetic transient matrix of load model and transformer model includes the following steps:
- the line model is a series circuit of resistance R and inductance L, so that the current vector of the circuit is The voltages in the direction of the current vector are respectively
- I m0 is the amplitude of the current in the previous frame
- I m0 ⁇ e j ⁇ is the current in the previous frame
- Predicted value of ⁇ T is the time interval between two adjacent frames
- circuit model is a series circuit of a resistor R and a capacitor C, so that the current vector of the circuit The voltages in the direction of the current vector are respectively
- I m0 is the amplitude of the current in the previous frame
- I m0 ⁇ e j ⁇ is the current in the previous frame
- Predicted value of ⁇ T is the time interval between two adjacent frames
- U 1m0 is the amplitude of the voltage at the left end of the previous frame, Is the left end voltage of the previous frame.
- U 2m0 is the amplitude of the voltage at the right end of the previous frame, Is the voltage at the right end of the previous frame Predicted value of
- the load model is a load circuit after the resistance R and the inductor L are connected in series, so that the current vector of the load circuit is The voltages across the load circuit are
- I m0 is the amplitude of the current in the previous frame
- I m0 ⁇ e j ⁇ is the current in the previous frame
- Predicted value of ⁇ T is the time interval between two adjacent frames
- the load model is a load circuit after the resistance R and the capacitor C are connected in series, so that the current vector of the load circuit is The voltages across the load circuit are
- I m0 is the amplitude of the current in the previous frame
- Is the current of the previous frame
- U m0 is the amplitude of the previous frame voltage, Is the previous frame voltage Predicted value of
- ⁇ T is the time interval between two adjacent frames
- a resistance R and an inductance L are connected in series on the series circuit of the generator G, so that the generator EMF vector
- the current vector of this series circuit is The voltages across the series circuit are
- I m0 is the amplitude of the current in the previous frame
- I m0 ⁇ e j ⁇ is the current in the previous frame
- Predicted value of ⁇ T is the time interval between two adjacent frames
- the transformer is a transformer
- the mutual inductance coefficient of the transformer is M
- the self-inductance coefficients of the two coils in the transformer are L1 and L2, respectively
- the current vector and voltage in the coil with the self-inductance coefficient L1 The vectors are with
- the current vector and voltage vector in the coil with a self-inductance coefficient of L2 are with
- I m10 is the amplitude of the current on the left end of the frame
- I m20 is the amplitude of the current on the right end of the frame, Is the previous frame current on the right Predicted value of
- ⁇ T is the time interval between two adjacent frames
- the present invention by solving the electromagnetic transient equations of the generator model, the line model, the load model and the transformer model existing in the power system network, a series of solving, collating and deforming the electromagnetic transient equations are carried out. Obtain the electromagnetic transient matrix.
- the matrix of lines, the matrix of loads, the matrix of generators and the matrix of transformers are all used.
- the electromagnetic transient matrices of different models are replaced with the above-mentioned matrices to realize the simulation of electromagnetic and electromechanical transients in order to ensure that the final calculation results are consistent with the actual situation of the power grid and can more truly reflect the changes of the power grid.
- FIG. 1 is a schematic diagram of a first line model in an electromagnetic electromechanical transient simulation algorithm based on a straight algorithm provided by the present invention
- FIG. 2 is a schematic diagram of a second line model in an electromagnetic electromechanical transient simulation algorithm based on a straight algorithm provided by the present invention
- FIG. 3 is a schematic diagram of a first load model in an electromagnetic electromechanical transient simulation algorithm based on a straight algorithm provided by the present invention
- FIG. 4 is a schematic diagram of a second load model in an electromagnetic electromechanical transient simulation algorithm based on a straight algorithm provided by the present invention
- FIG. 5 is a schematic diagram of a generator model in an electromagnetic electromechanical transient simulation algorithm based on a straight algorithm provided by the present invention
- FIG. 6 is a schematic diagram of a transformer model in an electromagnetic electromechanical transient simulation algorithm based on a straight algorithm provided by the present invention
- FIG. 7 is a schematic diagram of a line ⁇ type equivalent circuit provided by the present invention.
- FIG. 8 is a schematic diagram of a T-type equivalent circuit of a line provided by the present invention.
- the invention provides an electromagnetic electromechanical transient simulation algorithm based on a straight algorithm, and the electromagnetic transient matrix solved by the method can replace the application in the prior art "a straight algorithm based electromechanical transient simulation method of power system"
- the matrix in the power system network is mainly composed of one or any combination of generator, line, load and transformer models.
- ⁇ 2 ⁇ f is the angular velocity
- f is the frequency
- t is the time Is the initial phase.
- I m0 is the amplitude of the current in the previous frame
- I m0 ⁇ e j ⁇ is the current in the previous frame
- Predicted value of ⁇ T is the time interval between two adjacent frames
- the above-mentioned deformation method can refer to the patent number ZL201410142938.7.
- the name of the invention is: the calculation method used in the straight-chain and branch-chain three-phase symmetric multi-power non-loop network power system straight algorithm.
- the circuit model is a series circuit of resistor R and capacitor C, so that the current vector of the circuit is The voltages in the direction of the current vector are respectively The current vector is The direction is to That is, the voltages on the left and right ends of the circuit are respectively
- I m0 is the amplitude of the current in the previous frame
- I m0 ⁇ e j ⁇ is the current in the previous frame
- Predicted value of ⁇ T is the time interval between two adjacent frames
- U 1m0 is the amplitude of the voltage at the left end of the previous frame, Is the left end voltage of the previous frame.
- U 2m0 is the amplitude of the voltage at the right end of the previous frame, Is the voltage at the right end of the previous frame Predicted value of
- the above-mentioned deformation method can refer to the patent number ZL201410142938.7.
- the name of the invention is: the calculation method used in the straight-chain and branch-chain three-phase symmetric multi-power non-loop network power system straight algorithm.
- the current vector of the load circuit is The voltages across the load circuit are That is, the voltages on the left and right ends of the circuit are respectively
- I m0 is the amplitude of the current in the previous frame
- I m0 ⁇ e j ⁇ is the current in the previous frame
- Predicted value of ⁇ T is the time interval between two adjacent frames
- the above-mentioned deformation method can refer to the patent number ZL201410142938.7.
- the name of the invention is: the calculation method used in the straight-chain and branch-chain three-phase symmetric multi-power non-loop network power system straight algorithm.
- the load model is a load circuit with a resistor R and a capacitor C connected in series.
- the voltages across the load circuit are That is, the voltages on the left and right ends of the circuit are respectively among them,
- I m0 is the amplitude of the current in the previous frame
- Is the current of the previous frame
- U m0 is the amplitude of the previous frame voltage, Is the previous frame voltage Predicted value of
- ⁇ T is the time interval between two adjacent frames
- the above-mentioned deformation method can refer to the patent number ZL201410142938.7.
- the name of the invention is: the calculation method used in the straight-chain and branch-chain three-phase symmetric multi-power non-loop network power system straight algorithm.
- I m0 is the amplitude of the current in the previous frame
- I m0 ⁇ e j ⁇ is the current in the previous frame
- Predicted value of ⁇ T is the time interval between two adjacent frames
- the above-mentioned deformation method can refer to the patent number ZL201410142938.7.
- the name of the invention is: the calculation method used in the straight-chain and branch-chain three-phase symmetric multi-power non-loop network power system straight algorithm.
- the mutual inductance coefficient of the transformer is M
- the self-inductance coefficients of the two coils in the transformer are L1 and L2
- the current vector and voltage vector in the coil with the self-inductance coefficient L1 Are with
- the current vector and voltage vector in the coil with a self-inductance coefficient of L2 are with
- I m10 is the amplitude of the current on the left end of the frame
- I m20 is the amplitude of the current on the right end of the frame, Is the previous frame current on the right Predicted value of
- ⁇ T is the time interval between two adjacent frames
- the above-mentioned deformation method can refer to the patent number ZL201410142938.7.
- the name of the invention is: the calculation method used in the straight-chain and branch-chain three-phase symmetric multi-power non-loop network power system straight algorithm.
- the electromagnetic transient matrix of the line in the first line model is:
- the electromagnetic transient matrix of the line in the second line model is:
- the electromagnetic transient matrix for the load in the first load model is:
- the electromagnetic transient matrix for the load in the second load model is:
- the electromagnetic transient matrix for the generator model is:
- the electromagnetic transient matrix for the transformer model is:
- the name of the invention is: a method for electromechanical transient simulation of power system based on straight algorithm, through step A-step I to conduct electromechanical transient simulation of power system, in step A
- the reactance and susceptance of each node are determined according to fW , 0
- the initial matrix of all nodes is calculated;
- the load initial matrix is:
- the initial matrix of the line is:
- the initial matrix of the transformer is:
- the initial matrix of the generator is:
- the electromagnetic transient matrix in the load model is used to replace the load initial matrix; the electromagnetic transient matrix in the generator model is used to replace the generator initial matrix; and the electromagnetic transient matrix in the transformer model is used to replace the transformer
- the initial matrix and then continue to calculate based on step A-step I provided by the power flow direct calculation method to perform electromechanical transient simulation of the power system, the calculated results can realize the simulation of electromagnetic and electromechanical transient integration, And when ⁇ T is smaller, the electromagnetic transient effect is more obvious, and when ⁇ T is larger, the electromagnetic transient effect is weaker.
- the line initial matrix It can be equivalent to a line ⁇ type equivalent circuit or a line T type equivalent circuit;
- the electromagnetic transient matrix of the line distribution parameter model can be obtained by multiplying the following three electromagnetic transient matrices:
- the electromagnetic transient matrix of the line distribution parameter model can be obtained by multiplying the following three electromagnetic transient matrices:
- the application number is CN201810219284.1
- the name of the invention is: a load algorithm, line initialization matrix, transformer initialization matrix and generator initialization matrix in the electromechanical transient simulation method of the power system based on the straight algorithm are replaced accordingly
- the simulation calculation of electromagnetic electromechanical transient can be achieved.
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Abstract
一种基于直算法的电磁机电暂态仿真算法,属于电力系统仿真技术领域,在电力系统网络中包括发电机模型、线路模型、负载模型和变压器模型,分别计算发电机模型、线路模型、负载模型和变压器模型的电磁暂态矩阵,其包括以下步骤:(1)根据不同的模型分别求解对应的电磁暂态方程式;(2)将步骤(1)中的电磁暂态方程式整理成差分方程式;(3)对差分方程式进行整理并变形得到电磁暂态矩阵;并将电磁暂态矩阵代入基于直算法的电力系统机电暂态仿真方法中,以进行电磁暂态效应的仿真,以达到能够实现电磁、机电暂态于一体的仿真计算。
Description
本发明属于电力系统仿真技术领域,具体而言,涉及一种基于直算法的电磁机电暂态仿真算法。
电力系统中机电暂态过程和电磁暂态过程是两个用不同数学模型表征、具有不同时间常数的物理过程。在传统的电力系统分析工具中,通常对这两个过程分别进行数字仿真。相对于机电暂态仿真,电磁暂态下电力设备数学模型更复杂,所关注的动态时间常数更小,大大增加了仿真的计算量和计算时间,实现一定规模系统的实时数字仿真要困难得多。
电磁暂态过程数字仿真是用数值计算方法对电力系统中从数微秒至数秒之间的电磁暂态过程进行仿真模拟。电磁暂态过程仿真必须考虑输电线路分布参数特性和参数的频率特性、发电机的电磁和机电暂态过程以及一系列元件(避雷器、变压器、电抗器等)的非线性特性。因此,电磁暂态仿真的数学模型必须建立这些元件和系统的代数或微分、偏微分方程。一般采用的数值积分方法为隐式积分法。
由于电磁暂态仿真不仅要求对电力系统的动态元件采用详细的非线性模型,还要计及网络的暂态过程,也需采用微分方程描述,使得电磁暂态仿真程序的仿真规模受到了限制。一般进行电磁暂态仿真时,都要对电力系统进行等值化简。
机电暂态过程的仿真,主要研究电力系统受到大扰动后的暂态稳定和受到小扰动后的静态稳定性能。其中暂态稳定分析是研究电力系统受到诸如短路故障,切除线路、发电机、负荷,发电机失去励磁或者冲击性负荷等大扰动作用下,电力系统的动态行为和保持同步稳定运行的能力。
电力系统机电暂态仿真的算法是联立求解电力系统微分方程组和代数方程组,以获得物理量的时域解。微分方程组的求解方法主要有隐式梯形积分法、改进尤拉法、龙格-库塔法等,其中隐式梯形积分法由于数值稳定性好而得到越来越多的应用。代数方程组的求解方法主要采用适用于求解非线性代数方程组的牛顿法。按照微分方程和代数方程的求解顺序可分为交替解法和联立解法。
在专利号为ZL201410142938.7,发明名称为:一字链及支链式的三相对称 多电源非环网电力系统直算法中提供了一种运算结果精确、运算速度快的三相对称多电源非环网潮流直算法;
在申请号为CN201610783305.3,发明名称为:一种基于环网电力系统的直算方法,该专利主要解决了现有环网潮流算法应用的迭代法的计算结果误差大、不收敛、运算速度慢等问题;
而在申请号为CN201810219284.1,发明名称为:一种基于直算法的电力系统机电暂态仿真方法,其克服了传统仿真法的缺陷,无迭代、计算速度快、精度高且误差小,真实地反映了电网的变化特性,如各线路、负载和变压器的阻抗随着电网的频率变化而变化,电网中各发电机的频率也能按各自的规律动态地变化;
针对上述的现有技术中,虽然能够在传统的计算方法中基于直算法使计算结果更为精确,提升运算速度,但是,在上述三个专利文献所记载的技术方案中,并不能够直接实现电磁暂态的仿真计算。
发明内容
有鉴于此,为了解决现有技术存在的上述问题,本发明的目的在于提供一种基于直算法的电磁机电暂态仿真算法以达到能够实现电磁暂态于一体的仿真计算。
本发明所采用的技术方案为:一种基于直算法的电磁机电暂态仿真算法,在电力系统仿真中包括发电机模型、线路模型、负载模型和变压器模型,分别计算发电机模型、线路模型、负载模型和变压器模型的电磁暂态矩阵,其包括以下步骤:
(1)根据不同的模型分别求解对应的电磁暂态方程式;
(2)将步骤(1)中的电磁暂态方程式整理成差分方程式;
(3)对差分方程式进行整理得到电磁暂态矩阵;并将电磁暂态矩阵代入基于直算法的电力系统机电暂态仿真方法中,进行电磁机电暂态效应的仿真,以达到能够实现电磁、机电暂态于一体的仿真计算。
求解电磁暂态方程式:
整理成差分方程式:
整理得:
变形得到电磁暂态矩阵:
求解电磁暂态方程式:
两边微分:
整理成差分方程式:
变形得:
整理得:
最后得:
变形得到电磁暂态矩阵:
求解电磁暂态方程式:
整理为差分方程式:
整理得:
最后得:
变形得到电磁暂态矩阵:
求解电磁暂态方程式:
两边微分后得:
整理为差分方程式:
ΔT为相邻两帧之间的时间间隔;
整理得:
最后得:
变形得到电磁暂态矩阵:
整理为差分方程式:
整理得:
最后得:
变形得到电磁暂态矩阵:
进一步地,所述变压器模型中,设变压器为变压器,变压器的互感系数为M,变压器中两个线圈的自感系数分别为L1和L2,且自感系数为L1的线圈中的电流向量和电压向量分别为
和
而自感系数为L2的线圈中的电流向量和电压向量分别为
和
整理为差分方程式:
ΔT为相邻两帧之间的时间间隔;
变形为电磁暂态矩阵:
本发明的有益效果为:
1.在本发明中通过对电力系统网络中存在的发电机模型、线路模型、负载模型和变压器模型分别进行求解电磁暂态方程式,对电磁暂态方程式进行一系列的求解、整理以及变形,最终得到电磁暂态矩阵,在现有技术“一种基于直算法的电力系统机电暂态仿真方法”的运算过程中,均采用了线路的矩阵、负载的矩阵、发电机的矩阵以及变压器的矩阵,以不同模型的电磁暂态矩阵对应上述矩阵进行代替,以实现电磁、机电暂态于一体的仿真,以保证最终计算结果与电网的实际情况相符,并能够更加真实反映电网的变化。
图1是本发明提供的基于直算法的电磁机电暂态仿真算法中第一种线路模型的示意图;
图2是本发明提供的基于直算法的电磁机电暂态仿真算法中第二种线路模型的示意图;
图3是本发明提供的基于直算法的电磁机电暂态仿真算法中第一种负载模型的示意图;
图4是本发明提供的基于直算法的电磁机电暂态仿真算法中第二种负载模型的示意图;
图5是本发明提供的基于直算法的电磁机电暂态仿真算法中发电机模型的示意图;
图6是本发明提供的基于直算法的电磁机电暂态仿真算法中变压器模型的示意图;
图7是本发明提供的线路Π型等值电路示意图;
图8是本发明提供的线路T型等值电路示意图。
为使本发明实施例的目的、技术方案和优点更加清楚,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,所描述的实施例是本发明一部分实施例,而不是全部的实施例。通常在此处附图中描述和示出的本发明实施例的组件可以以各种不同的配置来布置和设计。
因此,以下对在附图中提供的本发明的实施例的详细描述并非旨在限制要求保护的本发明的范围,而是仅仅表示本发明的选定实施例。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。
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。
本发明提供了一种基于直算法的电磁机电暂态仿真算法,通过该方法所求解的电磁暂态矩阵能够代替现有技术“一种基于直算法的电力系统机电暂态仿真方法”中所运用的矩阵,在电力系统网络中,主要由发电机、线路、负载以及变压器模型中一种或任意几种组合而成,现结合附图,对各种不同的模型进行分别求解,具体如下:
求解电磁暂态方程式:
整理成差分方程式:
整理得:
变形得到电磁暂态矩阵:
上述变形方法可参照专利号为ZL201410142938.7,发明名称为:一字链及支链式的三相对称多电源非环网电力系统直算法中所运用的计算方法。
求解电磁暂态方程式:
对两边进行微分处理:
整理成差分方程式:
整理得:
整理得:
最后得:
变形得到电磁暂态矩阵:
上述变形方法可参照专利号为ZL201410142938.7,发明名称为:一字链及支链式的三相对称多电源非环网电力系统直算法中所运用的计算方法。
求解电磁暂态方程式:
整理为差分方程式:
整理得:
最后得:
变形得到电磁暂态矩阵:
上述变形方法可参照专利号为ZL201410142938.7,发明名称为:一字链及支链式的三相对称多电源非环网电力系统直算法中所运用的计算方法。
求解电磁暂态方程式:
两边微分后得:
整理为差分方程式:
ΔT为相邻两帧之间的时间间隔;
整理得:
最后得:
变形得到电磁暂态矩阵:
上述变形方法可参照专利号为ZL201410142938.7,发明名称为:一字链及支链式的三相对称多电源非环网电力系统直算法中所运用的计算方法。
整理为差分方程式:
整理得:
最后得:
变形得到电磁暂态矩阵:
上述变形方法可参照专利号为ZL201410142938.7,发明名称为:一字链及支链式的三相对称多电源非环网电力系统直算法中所运用的计算方法。
如图6所示,所述变压器模型中,设变压器的互感系数为M,变压器中两 个线圈的自感系数分别为L1和L2,且自感系数为L1的线圈中的电流向量和电压向量分别为
和
而自感系数为L2的线圈中的电流向量和电压向量分别为
和
整理为差分方程式:
ΔT为相邻两帧之间的时间间隔;
变形为电磁暂态矩阵:
上述变形方法可参照专利号为ZL201410142938.7,发明名称为:一字链及支链式的三相对称多电源非环网电力系统直算法中所运用的计算方法。
综上求解、整理以及变形,对于第一种线路模型中线路的电磁暂态矩阵为:
对于第二种线路模型中线路的电磁暂态矩阵为:
对于第一种负载模型中负载的电磁暂态矩阵为:
对于第二种负载模型中负载的电磁暂态矩阵为:
对于发电机模型的电磁暂态矩阵为:
对于变压器模型的电磁暂态矩阵为:
(一)、在申请号为CN201810219284.1,发明名称为:一种基于直算法的电力系统机电暂态仿真方法中,通过步骤A-步骤I进行电力系统机电暂态仿真,在步骤A中进行初始化电力系统参数时,步骤A4中设网上系统频率初始值为f
W,0=50Hz,根据f
W,0确定每一个节点的电抗和电纳,最后计算出所有节点的初始矩阵;
步骤A4具体包括以下过程:设电力系统中,在初始频率f
W,0=50Hz时,负载的电阻为R
i,0和电抗为X
i,0;线路每公里电阻为r
i,0、每公里电抗为x
i,0、每公里电导为g
i,0、每公里电纳为b
i,0和线路长度为l
i;变压器的电导为Gt
i,0、电纳为Bt
i,0、电阻为Rt
i,0、电抗为Xt
i,0,原边匝数为n
i,1和副边匝数为n
i,2;发电机的内阻为r′
i,0和电抗为x′
i,0;则各节点初始矩阵如下:
变压器初始矩阵为:
同理,以本实施例中具体求解中,以负载模型中电磁暂态矩阵代替负载初始矩阵;以发电机模型中电磁暂态矩阵代替发电机初始矩阵;以变压器模型中 电磁暂态矩阵代替变压器初始矩阵,再基于电力系统的潮流直算方法所提供的步骤A-步骤I进行继续计算,以进行电力系统机电暂态仿真,所计算的结果便能够实现电磁、机电暂态于一体的仿真,且当ΔT越小时,电磁暂态效应越明显,当ΔT越大时,电磁暂态效应越弱。
则线路分布参数模型的电磁暂态矩阵可由下面的三个电磁暂态矩阵相乘得到:
则线路分布参数模型的电磁暂态矩阵可由下面的三个电磁暂态矩阵相乘得到:
根据上述,将申请号为CN201810219284.1,发明名称为:一种基于直算法的电力系统机电暂态仿真方法中的负载初始矩阵、线路初始矩阵、变压器初始矩阵和发电机初始矩阵进行相应的替换后,参照“一种基于直算法的电力系统机电暂态仿真方法”中所公开的其他步骤继续进行运算,即可实现电磁机电暂态于一体的仿真计算。
本发明不局限于上述可选实施方式,任何人在本发明的启示下都可得出其他各种形式的产品,但不论在其形状或结构上作任何变化,凡是落入本发明权 利要求界定范围内的技术方案,均落在本发明的保护范围之内。
Claims (7)
- 一种基于直算法的电磁机电暂态仿真算法,在电力系统仿真中包括发电机模型、线路模型、负载模型和变压器模型,其特征在于,分别计算发电机模型、线路模型、负载模型和变压器模型的电磁暂态矩阵,其包括以下步骤:(1)根据不同的模型分别求解对应的电磁暂态方程式;(2)将步骤(1)中的电磁暂态方程式整理成差分方程式;(3)对差分方程式进行整理得到电磁暂态矩阵;并将电磁暂态矩阵代入基于直算法的电力系统机电暂态仿真方法中,进行电磁暂态效应的仿真。
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Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
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CN112234598A (zh) * | 2020-08-28 | 2021-01-15 | 国网天津市电力公司电力科学研究院 | 一种电磁暂态仿真初始化方法 |
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Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20040044503A1 (en) * | 2002-08-27 | 2004-03-04 | Mcconaghy Trent Lorne | Smooth operators in optimization of structures |
CN103956741A (zh) * | 2014-04-10 | 2014-07-30 | 邓宏伟 | 一字链及支链式的三相对称多电源非环网电力系统直算法 |
CN106451456A (zh) * | 2016-08-30 | 2017-02-22 | 邓宏伟 | 一种基于环网电力系统的直算方法 |
CN108365629A (zh) * | 2018-03-16 | 2018-08-03 | 邓宏伟 | 一种基于直算法的电力系统机电暂态仿真方法 |
CN108536925A (zh) * | 2018-03-21 | 2018-09-14 | 武汉大学 | 一种隔离型动态全过程实时混合仿真接口系统 |
CN109063408A (zh) * | 2018-10-31 | 2018-12-21 | 邓宏伟 | 一种基于直算法的电磁机电暂态仿真算法 |
Family Cites Families (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20110257943A1 (en) * | 2010-04-16 | 2011-10-20 | Texas Instruments Incorporated | Node-based transient acceleration method for simulating circuits with latency |
CN103077268B (zh) * | 2012-12-27 | 2015-08-19 | 天津大学 | 面向电力系统电磁暂态仿真的状态空间自动建模方法 |
CN105224754B (zh) * | 2015-10-14 | 2018-08-10 | 清华大学 | 一种基于插值补偿电流开关模型的电力电子仿真方法 |
CN106372339B (zh) * | 2016-09-05 | 2019-08-09 | 清华大学 | 电力电子化电力系统的多速率仿真方法及装置 |
-
2018
- 2018-10-31 CN CN201811285344.6A patent/CN109063408B/zh active Active
-
2019
- 2019-10-15 WO PCT/CN2019/111295 patent/WO2020088245A1/zh active Application Filing
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20040044503A1 (en) * | 2002-08-27 | 2004-03-04 | Mcconaghy Trent Lorne | Smooth operators in optimization of structures |
CN103956741A (zh) * | 2014-04-10 | 2014-07-30 | 邓宏伟 | 一字链及支链式的三相对称多电源非环网电力系统直算法 |
CN106451456A (zh) * | 2016-08-30 | 2017-02-22 | 邓宏伟 | 一种基于环网电力系统的直算方法 |
CN108365629A (zh) * | 2018-03-16 | 2018-08-03 | 邓宏伟 | 一种基于直算法的电力系统机电暂态仿真方法 |
CN108536925A (zh) * | 2018-03-21 | 2018-09-14 | 武汉大学 | 一种隔离型动态全过程实时混合仿真接口系统 |
CN109063408A (zh) * | 2018-10-31 | 2018-12-21 | 邓宏伟 | 一种基于直算法的电磁机电暂态仿真算法 |
Cited By (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN112084624A (zh) * | 2020-07-31 | 2020-12-15 | 清华大学 | 电磁-机电混合仿真电磁暂态侧接口功率计算方法与装置 |
CN112234598A (zh) * | 2020-08-28 | 2021-01-15 | 国网天津市电力公司电力科学研究院 | 一种电磁暂态仿真初始化方法 |
CN112234598B (zh) * | 2020-08-28 | 2024-04-23 | 国网天津市电力公司电力科学研究院 | 一种电磁暂态仿真初始化方法 |
CN113076675A (zh) * | 2021-04-12 | 2021-07-06 | 中国电子科技集团公司第三十三研究所 | 一种气垫登陆艇电磁环境效应仿真设计方法 |
CN113076675B (zh) * | 2021-04-12 | 2022-11-08 | 中国电子科技集团公司第三十三研究所 | 一种气垫登陆艇电磁环境效应仿真设计方法 |
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CN113536589B (zh) * | 2021-07-30 | 2023-08-04 | 广东电网有限责任公司广州供电局 | 一种交流电网的电磁暂态建模方法和系统 |
WO2024082163A1 (zh) * | 2022-10-19 | 2024-04-25 | 云南电网有限责任公司电力科学研究院 | 一种变压器电磁暂态仿真方法、计算机设备及存储介质 |
CN116722563A (zh) * | 2023-05-30 | 2023-09-08 | 杭州盛星能源技术有限公司 | 一种基于动态相量的电磁暂态仿真频域扩展方法及装置 |
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