Harmonic Emissions of Power Electronic Devices Under Different Transmission Network Operating Conditions

被引:15
|
作者
Bozicek, Ambroz [1 ]
Kilter, Jako [2 ]
Sarnet, Tanel [2 ]
Papic, Igor [1 ]
Blazic, Bostjan [1 ]
机构
[1] Univ Ljubljana, Fac Elect Engn, Ljubljana 1000, Slovenia
[2] Tallinn Univ Technol, Dept Elect Power Engn & Mechatron, EE-12616 Tallinn, Estonia
基金
欧盟地平线“2020”;
关键词
Harmonic analysis; load modeling; power electronics (PE); power quality; power system harmonics; ADMITTANCE MATRIX;
D O I
10.1109/TIA.2018.2808478
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Harmonic emissions of power electronic (PE) devices connected to transmission networks are introducing new and rising trends of harmonic distortion. Analyses, which focus on assessing the harmonic levels in PE-rich power networks of the future, are mostly based on digital simulations, which require accurate models of the power system and connected devices. The simulations are usually performed with the use of electro-magnetic transient (EMT) models, resulting in long simulation times or the use of oversimplified load-flow models. In this paper, we propose a methodology that can be used to define accurate frequency-domain simulation models of PE devices. The models are derived by frequency-dependent multiparameter scanning. The resulting models can be employed for harmonic load-flow simulations in different network and PE-device operating conditions. They enable the assessment of the impact of frequency-dependent network-impedance characteristics and, moreover, the effect of cross coupling between different frequency components. The analysis is focused on high-power high-voltage PE devices, which cannot be easily measured or analyzed for harmonic characteristics. Therefore, the methodology requires detailed EMT models of the devices, which are analyzed within different operating conditions. The accurate equivalent models of PE devices represent a crucial element within the context of harmonic emission studies in large transmission networks.
引用
收藏
页码:5216 / 5226
页数:11
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