CN112084679B - A Modeling Method of Equivalent Magnetic Circuit of Electromagnetic Actuator Considering Inhomogeneity of Eddy Current Distribution - Google Patents
A Modeling Method of Equivalent Magnetic Circuit of Electromagnetic Actuator Considering Inhomogeneity of Eddy Current Distribution Download PDFInfo
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Abstract
本发明的目的在于提供一种考虑涡流分布不均匀性电磁执行器等效磁路建模方法,包括如下步骤:根据电磁执行器的结构进行分区划分A~D,定义各区上第一层和第n层涡电流分别为iR11和iR1n,计算第一层和第n层对应的涡电阻,定义电磁执行器铁芯和衔铁之间气隙部分的等效电流为igk,定义A~D区漏磁部分的等效电感为Lair1~Lair4,计算A~D区相邻两薄层之间的磁链,计算干路电流i,从而得到电磁执行器磁通φ。本发明实现了已有方法无法解决铁芯磁性材料的非线性磁化和磁饱和现象,特别是磁场内涡流效应的考虑。本发明提出的建模方法可以用于电磁执行器动态性能的准确预测。
The purpose of the present invention is to provide a method for modeling the equivalent magnetic circuit of an electromagnetic actuator considering the inhomogeneity of eddy current distribution, including the following steps: dividing A to D according to the structure of the electromagnetic actuator, and defining the first layer and the first layer in each area. The eddy currents of the n layers are i R11 and i R1n respectively , calculate the eddy resistances corresponding to the first layer and the nth layer, define the equivalent current of the air gap between the electromagnetic actuator core and the armature as i gk , define A~D The equivalent inductance of the leakage magnetic part of the area is L air1 ~L air4 , calculate the flux linkage between the two adjacent thin layers in the A~D area, calculate the main circuit current i, and obtain the magnetic flux φ of the electromagnetic actuator. The invention realizes that the existing methods cannot solve the nonlinear magnetization and magnetic saturation phenomena of the iron core magnetic material, especially the consideration of the eddy current effect in the magnetic field. The modeling method proposed by the invention can be used for accurate prediction of the dynamic performance of the electromagnetic actuator.
Description
技术领域technical field
本发明涉及的是一种电磁执行器,具体地说是高压共轨系统的电磁执行器。The invention relates to an electromagnetic actuator, in particular to an electromagnetic actuator of a high-voltage common rail system.
背景技术Background technique
高速电磁执行器是高压共轨系统的核心控制部件,直接决定共轨系统的喷射特性,从而影响柴油机的动力性和排放性。通常,采用三维有限元方法进行电磁执行器的设计优化,然而三维电磁计算耗时较长,无法实现对不同方案的快速计算对比。更为突出的问题是,三维有限元方法无法实现电磁执行器和高压共轨系统的液压部件、机械部件等耦合计算,这导致无法准确预测电磁执行器动态性能对共轨系统喷射特性的影响。因此,计算速度快、计算精度高的基于等效磁路法的一维电磁模型得到了广泛的发展。发明专利《基于等效磁路法的永磁同步直线电机建模与特性分析方法》在进行建模时,把永磁同步电机磁路分为直线电机初级部分磁路和气隙、电机次级部分磁路,然而模型不考虑铁芯磁饱和,这违背了真实的磁性材料存在的磁饱和特性。发明专利《一种永磁同步电机失磁故障等效磁路模型建立方法》在建模时忽略定子铁芯的磁阻和转子磁阻,并且假设永磁同步电机的硅钢片为不饱和状态,从而建立简化等效磁路模型,这种假设使得上述的模型无法准确预测在磁饱和下永磁电机的工作特性,模型具有一定的局限性。实际上,在高速电机或是高速电磁阀等电磁执行器的等效磁路模型中,是需要考虑到磁场的饱和特性和集肤效应导致的涡流在铁芯材料沿着径向分布的不均匀性。The high-speed electromagnetic actuator is the core control component of the high-pressure common rail system, which directly determines the injection characteristics of the common rail system, thereby affecting the power and emission performance of the diesel engine. Usually, the 3D finite element method is used to optimize the design of electromagnetic actuators. However, the 3D electromagnetic calculation takes a long time, and it is impossible to achieve rapid calculation and comparison of different schemes. The more prominent problem is that the three-dimensional finite element method cannot realize the coupling calculation of the electromagnetic actuator and the hydraulic components and mechanical components of the high-pressure common rail system, which makes it impossible to accurately predict the influence of the dynamic performance of the electromagnetic actuator on the injection characteristics of the common rail system. Therefore, the one-dimensional electromagnetic model based on the equivalent magnetic circuit method with fast calculation speed and high calculation accuracy has been widely developed. The invention patent "Modeling and Characteristic Analysis Method of Permanent Magnet Synchronous Linear Motor Based on Equivalent Magnetic Circuit Method" When modeling, the magnetic circuit of permanent magnet synchronous motor is divided into the primary part of the linear motor, the air gap, and the secondary part of the motor. The magnetic circuit, however, the model does not take into account the magnetic saturation of the iron core, which violates the magnetic saturation characteristics that exist in real magnetic materials. The invention patent "A Method for Establishing an Equivalent Magnetic Circuit Model of Permanent Magnet Synchronous Motor Loss of Field Failure" ignores the reluctance of the stator core and the rotor reluctance when modeling, and assumes that the silicon steel sheet of the permanent magnet synchronous motor is in an unsaturated state, Therefore, a simplified equivalent magnetic circuit model is established. This assumption makes the above model unable to accurately predict the working characteristics of the permanent magnet motor under magnetic saturation, and the model has certain limitations. In fact, in the equivalent magnetic circuit model of electromagnetic actuators such as high-speed motors or high-speed solenoid valves, it is necessary to take into account the saturation characteristics of the magnetic field and the uneven distribution of eddy currents in the radial direction of the core material caused by the skin effect. sex.
发明内容SUMMARY OF THE INVENTION
本发明的目的在于提供克服现有的电磁执行器等效磁路法没有考虑铁芯磁特性和涡流特性等不足的一种考虑涡流分布不均匀性电磁执行器等效磁路建模方法。The purpose of the present invention is to provide a method for modeling the equivalent magnetic circuit of an electromagnetic actuator considering the inhomogeneity of the eddy current distribution, which overcomes the shortcomings of the existing electromagnetic actuator equivalent magnetic circuit method that does not consider the iron core magnetic characteristics and eddy current characteristics.
本发明的目的是这样实现的:The object of the present invention is achieved in this way:
本发明一种考虑涡流分布不均匀性电磁执行器等效磁路建模方法,其特征是:A method for modeling an equivalent magnetic circuit of an electromagnetic actuator considering the inhomogeneity of eddy current distribution in the present invention is characterized in that:
(1)根据电磁执行器的结构进行分区划分,定义内磁极部分为A区、外磁极部分为B区、连接内外磁极的位于线圈绕组上面的区域为C区、衔铁部分为D区;对上述定义的四个区域在径向方向进行n层等厚度的薄片划分,并假设在每层铁芯薄片内的涡流为均匀分布;(1) According to the structure of the electromagnetic actuator, the division is carried out, and the inner magnetic pole part is defined as the A area, the outer magnetic pole part is defined as the B area, the area on the coil winding connecting the inner and outer magnetic poles is the C area, and the armature part is the D area; The defined four regions are divided into n layers of equal thickness slices in the radial direction, and it is assumed that the eddy current in each layer of iron core slices is uniformly distributed;
(2)定义A区上第一层和第n层涡电流分别为iR11和iR1n,第一层和第n 层对应的涡电阻分别为R11和R1n,同理,B区、C区、D区上涡电流从第一层到第n层为iR21~iR2n、iR31~iR3n、iR41~iR4n,各薄层涡电阻为R11~R1n、R21~ R2n、R31~R3n、R41~R4n,薄层内涡电阻计算公式为:(2) Define the eddy currents of the first layer and the nth layer on the A area as i R11 and i R1n respectively , and the eddy resistances corresponding to the first layer and the nth layer are R 11 and R 1n respectively. Similarly, the B area, C The eddy currents in zone and D zone from the first layer to the nth layer are i R21 ~i R2n , i R31 ~i R3n , i R41 ~i R4n , and the eddy resistances of each thin layer are R 11 ~R 1n , R 21 ~ R 2n , R 31 ~R 3n , R 41 ~R 4n , the calculation formula of the eddy resistance in the thin layer is:
上式中,m=1~4,q=1~n,ρm为材料的电阻率,N是线圈匝数,lmq为涡流的流通距离,Smq为涡流的流通面积;In the above formula, m=1~4, q=1~n, ρ m is the resistivity of the material, N is the number of turns of the coil, l mq is the circulation distance of the eddy current, and S mq is the circulation area of the eddy current;
(3)定义电磁执行器铁芯和衔铁之间气隙部分的等效电流为igk:(3) Define the equivalent current of the air gap between the electromagnetic actuator core and the armature as i gk :
上式中,k=1或2,μ0是真空磁导率,Sgk和φgk分别是气隙部分的有效磁通面积和磁通量,lgk是气隙部分磁通的距离;In the above formula, k=1 or 2, μ 0 is the vacuum permeability, S gk and φ gk are the effective magnetic flux area and magnetic flux of the air gap part, respectively, and l gk is the distance of the magnetic flux of the air gap part;
(4)在考虑到电磁执行器漏磁现象时,定义A~D区漏磁部分的等效电感为Lair1~Lair4,其计算公式为:(4) When considering the magnetic flux leakage phenomenon of electromagnetic actuators, define the equivalent inductances of the magnetic flux leakage parts of the A to D regions as L air1 ~L air4 , and the calculation formula is:
上式中,x=1~4,Sm为磁通面积,lm为磁通距离;根据在上述四个漏磁区域的电感和电流的关系,计算得到有效电流为:In the above formula, x=1~4, S m is the magnetic flux area, and l m is the magnetic flux distance; according to the relationship between the inductance and current in the above four magnetic leakage regions, the effective current is calculated as:
上式中,E为加载到电磁执行器上的驱动电压,RR为驱动电路干路电阻,i为驱动电路干路电流;In the above formula, E is the driving voltage loaded on the electromagnetic actuator, RR is the main circuit resistance of the driving circuit, and i is the main circuit current of the driving circuit;
(5)计算A~D区相邻两薄层之间的磁链,计算公式为:(5) Calculate the magnetic linkage between the two adjacent thin layers in the A-D area, and the calculation formula is:
ψmp=∫iRmp·Rmp-iRm(p+1)·Rm(p+1)dt m=1~4,p=1~(n-1)ψ mp =∫i Rmp ·R mp -i Rm(p+1) ·R m(p+1) dt m=1~4,p=1~(n-1)
上式中,相邻两薄层的涡流iRmp和iRm(p+1)由基尔霍夫定律求得;根据上式求得的磁链计算得到相邻两个薄层之间的磁感应强度为:In the above formula, the eddy currents i Rmp and i Rm(p+1) of two adjacent thin layers are obtained by Kirchhoff's law; the magnetic induction between two adjacent thin layers can be obtained by calculating the flux linkage obtained by the above formula. The strength is:
上式中,Smp为磁感线穿过的有效面积;利用数据插值法求得磁化曲线中磁感应强度Bmp对应的磁场强度Hmp,进而计算出相邻两薄层之间等效电感对应的电流Imp:In the above formula, S mp is the effective area that the magnetic field line passes through; the magnetic field intensity H mp corresponding to the magnetic field intensity B mp in the magnetization curve is obtained by the data interpolation method, and then the equivalent inductance corresponding to the two adjacent thin layers is calculated. The current Imp :
(6)根据基尔霍夫定律,由公式 ψmp=∫iRmp·Rmp-iRm(p+1)·Rm(p+1)dt m=1~4,p=1~(n-1)计算得到干路电流i,从而得到电磁执行器磁通φ:(6) According to Kirchhoff's law, the formula ψ mp =∫i Rmp ·R mp -i Rm(p+1) ·R m(p+1) dt m=1~4,p=1~(n-1) The main circuit current i is obtained by calculating Electromagnetic actuator magnetic flux φ:
本发明的优势在于:本发明实现了已有方法无法解决铁芯磁性材料的非线性磁化和磁饱和现象,特别是磁场内涡流效应的考虑。本发明提出的建模方法可以用于电磁执行器动态性能的准确预测。The advantages of the present invention are: the present invention realizes the non-linear magnetization and magnetic saturation phenomena of the iron core magnetic material which cannot be solved by the existing methods, especially the consideration of the eddy current effect in the magnetic field. The modeling method proposed by the invention can be used for accurate prediction of the dynamic performance of the electromagnetic actuator.
附图说明Description of drawings
图1为电磁执行器分区分层示意图;Fig. 1 is the schematic diagram of electromagnetic actuator partition and layering;
图2为构建的电磁执行器等效磁路示意图;Figure 2 is a schematic diagram of the equivalent magnetic circuit of the constructed electromagnetic actuator;
图3为本发明的流程图。Figure 3 is a flow chart of the present invention.
具体实施方式Detailed ways
下面结合附图举例对本发明做更详细地描述:The present invention will be described in more detail below in conjunction with the accompanying drawings:
结合图1-3,本发明具体步骤如下:1-3, the specific steps of the present invention are as follows:
(1)根据电磁执行器的结构进行分区划分,定义内磁极部分为A区,外磁极部分为B区,连接内外磁极的位于线圈绕组上面的区域为C区,衔铁部分为 D区。如图1所示,对上述定义的四个区域在径向方向进行六层等厚度的薄片划分,并假设在每层铁芯薄片内的涡流为均匀分布,图2为划分后构建的电磁执行器等效磁路结构图。(1) According to the structure of the electromagnetic actuator, the division is divided, and the inner magnetic pole part is defined as the A area, the outer magnetic pole part is the B area, the area above the coil winding connecting the inner and outer magnetic poles is the C area, and the armature part is D area. As shown in Figure 1, the above-defined four regions are divided into six layers of equal thickness in the radial direction, and it is assumed that the eddy current in each layer of the core sheet is uniformly distributed. Figure 2 shows the electromagnetic implementation constructed after the division. Equivalent magnetic circuit structure diagram of the device.
(2)定义A区上第一层和第六层涡电流分别为iR11和iR16,而第一层和第六层对应的涡电阻分别为R11和R16,同理,B区、C区、D区上涡电流从第一层到第六层为iR21~iR26、iR31~iR36、iR41~iR46,各薄层涡电阻为R11~R16、 R21~R26、R31~R36、R41~R46。薄层内涡电阻计算公式为:(2) Define the eddy currents of the first layer and the sixth layer on the A area as i R11 and i R16 respectively, and the eddy resistances corresponding to the first layer and the sixth layer are R 11 and R 16 respectively. Similarly, the B area, The eddy currents on the C area and the D area from the first layer to the sixth layer are i R21 ~i R26 , i R31 ~i R36 , i R41 ~i R46 , and the eddy resistance of each thin layer is R 11 ~R 16 , R 21 ~ R 26 , R 31 to R 36 , and R 41 to R 46 . The formula for calculating the eddy resistance in the thin layer is:
上式中,m=1~4,q=1~6,ρm为材料的电阻率,N是线圈匝数,lmq为涡流的流通距离,Smq为涡流的流通面积。In the above formula, m=1~4, q=1~6, ρ m is the resistivity of the material, N is the number of turns of the coil, l mq is the circulation distance of the eddy current, and S mq is the circulation area of the eddy current.
(3)定义电磁执行器铁芯和衔铁之间气隙部分的等效电流为igk,其计算公式为:(3) Define the equivalent current of the air gap between the electromagnetic actuator core and the armature as i gk , and its calculation formula is:
上式中,k=1或2,μ0是真空磁导率,Sgk和φgk分别是气隙部分的有效磁通面积和磁通量,lgk是气隙部分磁通的距离。In the above formula, k=1 or 2, μ 0 is the vacuum permeability, S gk and φ gk are the effective magnetic flux area and magnetic flux of the air gap part, respectively, and l gk is the distance of the magnetic flux of the air gap part.
(4)在考虑到电磁执行器漏磁现象时,定义A~D区漏磁部分的等效电感为Lair1~Lair4,其计算公式为:(4) When considering the magnetic flux leakage phenomenon of electromagnetic actuators, define the equivalent inductances of the magnetic flux leakage parts of the A to D regions as L air1 ~L air4 , and the calculation formula is:
上式中,x=1~4,Sm为磁通面积,lm为磁通距离。根据在上述四个漏磁区域的电感和电流的关系,计算得到有效电流为:In the above formula, x=1~4, S m is the magnetic flux area, and l m is the magnetic flux distance. According to the relationship between the inductance and the current in the above four magnetic leakage regions, the effective current is calculated as:
上式中,E为加载到电磁执行器上的驱动电压,RR为驱动电路干路电阻。i为驱动电路干路电流。In the above formula, E is the driving voltage loaded on the electromagnetic actuator, and RR is the main circuit resistance of the driving circuit. i is the main circuit current of the drive circuit.
(5)计算A~D区相邻两薄层之间的磁链,计算公式为:(5) Calculate the magnetic linkage between the two adjacent thin layers in the A-D area, and the calculation formula is:
ψmp=∫iRmp·Rmp-iRm(p+1)·Rm(p+1)dt m=1~4,p=1~5 (5)ψ mp =∫i Rmp ·R mp -i Rm(p+1) ·R m(p+1) dt m=1~4,p=1~5 (5)
上式中,相邻两薄层的涡流iRmp和iRm(p+1)由基尔霍夫定律求得。根据公式(5) 求得的磁链计算得到相邻两个薄层之间的磁感应强度为:In the above formula, the eddy currents i Rmp and i Rm(p+1) of two adjacent thin layers are obtained by Kirchhoff's law. According to the flux linkage obtained by formula (5), the magnetic induction intensity between two adjacent thin layers is calculated as:
上式中,Smp为磁感线穿过的有效面积。利用数据插值法求得磁化曲线中磁感应强度Bmp对应的磁场强度Hmp,进而计算出相邻两薄层之间等效电感对应的电流Imp:In the above formula, S mp is the effective area through which the magnetic field lines pass. The data interpolation method is used to obtain the magnetic field intensity H mp corresponding to the magnetic induction intensity B mp in the magnetization curve, and then the current I mp corresponding to the equivalent inductance between two adjacent thin layers is calculated:
(6)根据基尔霍夫定律,由公式(3)、(4)、(5)计算得到干路电流i,从而得到电磁执行器磁通φ:(6) According to Kirchhoff's law, the main circuit current i is calculated by formulas (3), (4) and (5), so as to obtain the magnetic flux φ of the electromagnetic actuator:
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