Analysis and Optimization of Magnetic Field Characteristics for Vacuum Interrupter with Horseshoe-shaped Axial Magnetic Field Contacts Based on Response Surface Method
|更新时间:2025-04-26
|
Analysis and Optimization of Magnetic Field Characteristics for Vacuum Interrupter with Horseshoe-shaped Axial Magnetic Field Contacts Based on Response Surface Method
High VoltageApparatusVol. 53, Issue 3, Pages: 90-96(2017)
WANG Zihan, LI Haomin, WANG Jianhua, et al. Analysis and Optimization of Magnetic Field Characteristics for Vacuum Interrupter with Horseshoe-shaped Axial Magnetic Field Contacts Based on Response Surface Method[J]. High voltageapparatus, 2017, 53(3): 90-96.
WANG Zihan, LI Haomin, WANG Jianhua, et al. Analysis and Optimization of Magnetic Field Characteristics for Vacuum Interrupter with Horseshoe-shaped Axial Magnetic Field Contacts Based on Response Surface Method[J]. High voltageapparatus, 2017, 53(3): 90-96. DOI: 10.13296/j.1001-1609.hva.2017.03.014.
Analysis and Optimization of Magnetic Field Characteristics for Vacuum Interrupter with Horseshoe-shaped Axial Magnetic Field Contacts Based on Response Surface Method
通过多目标优化的方式对灭弧室磁场特性进行优化。得到了各优化指标随触头结构参数的变化趋势及灭弧室磁场特性最优时的触头结构参数组合——铁片外径90 mm
内外径差55 mm
铁片间槽口夹角差值8.54°。较优化前
将电流峰值时纵向磁感应强度由633.3 mT提高至713.3 mT
将有效磁场区域宽度由25.2 mm增加至25.9 mm
将磁场滞后时间由1.16 ms缩短至0.77 ms。
Abstract
To improve the characteristics of the electric field in a vacuum interrupter with horseshoe-shaped axial magnetic field contacts
the response surface method is employed for optimization. Three contact parameters
i.e.
the outer diameter of the iron plate(d)
the difference between the outer and inner diameters of the iron plate(s)
and the difference of the slot angle between each iron plate(θ)
are chosen as the optimizing parameters. The axial magnetic flux density at current peak
the width of effective magnetic area and the phase shift time are chosen as the optimizing objectives. A 3-D finite element model of the contact is built
and simulation is carried out based on the central composite design method. Simulation results are analyzed by the response surface method
and the magnetic field characteristics are optimized by multiple objective optimization. As a result
the optimal values of d
s and θ are determined as90 mm
55 mm and 8.54°
respectively; the axial magnetic flux density at current peak increases from633.3 to 713.3 m T; the width of effective magnetic area increases from 25.2 to 25.9 mm
and the phase shift time decreases from 1.16 to 0.77 ms.