中国电力 ›› 2024, Vol. 57 ›› Issue (10): 190-198.DOI: 10.11930/j.issn.1004-9649.202408058
周洋1(), 黄德志2(
), 李培栋1(
), 冀凯琳1(
), 刘学峰1(
), 谭洪3(
)
收稿日期:
2024-08-15
出版日期:
2024-10-28
发布日期:
2024-10-25
作者简介:
周洋(1991—),女,硕士,主要从事电网工程经济评价,E-mail:1124108352@qq.com基金资助:
Yang ZHOU1(), Dezhi HUANG2(
), Peidong LI1(
), Kailin JI1(
), Xuefeng LIU1(
), Hong TAN3(
)
Received:
2024-08-15
Online:
2024-10-28
Published:
2024-10-25
Supported by:
摘要:
考虑到光伏逆变电源接入低压配电网的多样接入方式和复杂控制策略,建立了光伏逆变电源的三相电压与功率相对于中性点的控制模型。在此基础上,进一步提出了一个综合考量平衡端点相位不对称性以及光伏逆变电源接入因素的低压配电网三相潮流计算模型。为了验证该模型的有效性和准确性,在经过修正的IEEE 13节点测试系统上进行了仿真实验。仿真结果表明:所构建的模型能够精确、高效地计算包含光伏逆变电源在内的低压配电网三相潮流,为低压配电网的规划与运行提供了有力的理论支持和技术手段。
周洋, 黄德志, 李培栋, 冀凯琳, 刘学峰, 谭洪. 考虑平衡端点相位不对称及光伏接入的低压配电网三相潮流模型[J]. 中国电力, 2024, 57(10): 190-198.
Yang ZHOU, Dezhi HUANG, Peidong LI, Kailin JI, Xuefeng LIU, Hong TAN. A Three-Phase Power Flow Model for Low-Voltage Distribution Networks Considering Balanced Bus Phase Asymmetry and Photovoltaic Access[J]. Electric Power, 2024, 57(10): 190-198.
潮流结果 | 相别 | 方案1) | 方案2) | 方案3) | ||||||||
三相功率/ (MV·A) | A | 1.0209+ j0.7029 | 1.0799+ j0.5748 | 1.0799+ j0.5748 | –5.56% | 0 | ||||||
B | 0.9464+ j0.6018 | 1.0134+ j0.7116 | 1.0134+ j0.7116 | –6.61% | 0 | |||||||
C | 1.2963+ j1.0521 | 1.1680+ j1.0629 | 1.1680+ j1.0629 | 10.96% | 0 | |||||||
三相相角/(°) | A | 0 | 0 | 0 | — | — | ||||||
B | –120 | –120 | –120 | — | — | |||||||
C | –240 | –192 | –192 | — | — | |||||||
收敛次数/次 | — | 5 | 6 | 8 | — | — | ||||||
计算时间/s | — | 0.0405 | 0.0473 | 0.0715 | — | — |
表 1 3种方案计算下的平衡端点潮流
Table 1 Balanced bus power flow under three cases
潮流结果 | 相别 | 方案1) | 方案2) | 方案3) | ||||||||
三相功率/ (MV·A) | A | 1.0209+ j0.7029 | 1.0799+ j0.5748 | 1.0799+ j0.5748 | –5.56% | 0 | ||||||
B | 0.9464+ j0.6018 | 1.0134+ j0.7116 | 1.0134+ j0.7116 | –6.61% | 0 | |||||||
C | 1.2963+ j1.0521 | 1.1680+ j1.0629 | 1.1680+ j1.0629 | 10.96% | 0 | |||||||
三相相角/(°) | A | 0 | 0 | 0 | — | — | ||||||
B | –120 | –120 | –120 | — | — | |||||||
C | –240 | –192 | –192 | — | — | |||||||
收敛次数/次 | — | 5 | 6 | 8 | — | — | ||||||
计算时间/s | — | 0.0405 | 0.0473 | 0.0715 | — | — |
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