使用基态机器学习模型加速交流潮流事故分析
Expediting AC Contingency Analysis using a Basecase Machine Learning Model
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中文总结 AI 辅助
提出一种定点框架,复用仅基于基态拓扑训练的单一机器学习模型预测非关键单线停运后交流潮流状态,在6717节点系统上验证了收敛性和精度,兼顾直流求解器速度与牛顿-拉夫逊精度。
中文摘要 AI 辅助
在日益多变的运行条件下,电网规划和运行需要对大量线路停运进行快速且准确的交流潮流(AC-PF)事故分析。虽然机器学习模型可以加速这些计算,但现有方法通常需要针对不同事故训练单独的模型,或使用来自多种拓扑结构的数据训练单一模型。这两种方法都会产生大量的离线数据生成和训练成本。为解决这一问题,本文提出了一种定点框架,该框架复用仅基于基态拓扑数据训练的单一机器学习模型,以预测任何非关键单线停运后的事故后交流潮流状态。我们在直流模型近似下分析了所提方法的收敛性,并根据网络参数推导了其收敛速率。作为附带结果,我们证明了非关键线路的功率传输分配因子(PTDF)的幅值小于1。我们进一步刻画了机器学习训练区域,以适应定点迭代中遇到的功率因数规格,并推导了事故后状态估计的机器学习预测误差界限。在6717节点合成德克萨斯系统上的数值测试表明,该方法在所有非关键单线停运情况下均能收敛,且预测误差与基态情况保持接近。所提出的框架在直流求解器的速度和牛顿-拉夫逊法的精度之间提供了有利的权衡。
英文摘要
Grid planning and operation under increasingly variable operating conditions require fast and accurate AC power flow (AC-PF) contingency analysis for numerous line outages. While ML models can accelerate these computations, existing approaches often require either training separate models for different contingencies or a single model using data from multiple topologies. Both approaches incur substantial offline data generation and training costs. To address this gap, this work proposes a fixed-point framework that reuses a single ML model trained exclusively on basecase topology data to predict post-contingency AC-PF states under any non-critical single-line outage. We analyze the proposed method's convergence under the DC model approximation and derive its convergence rate in terms of network parameters. As a side result, we show that power transfer distribution factors (PTDFs) for non-critical lines have magnitudes less than one. We further characterize the ML training region to accommodate PF specifications encountered during fixed-point iterations and derive bounds on ML prediction errors for post-contingency state estimates. Numerical tests on a 6,717-bus synthetic Texas system demonstrate convergence across all non-critical single-line outages, with prediction errors remaining close to those of basecase. The proposed framework offers a favorable tradeoff between the speed of DC solvers and Newton-Raphson accuracy.