CN106208555B - A kind of extended method of built-in brshless DC motor pole embrace - Google Patents

A kind of extended method of built-in brshless DC motor pole embrace Download PDF

Info

Publication number
CN106208555B
CN106208555B CN201610811230.5A CN201610811230A CN106208555B CN 106208555 B CN106208555 B CN 106208555B CN 201610811230 A CN201610811230 A CN 201610811230A CN 106208555 B CN106208555 B CN 106208555B
Authority
CN
China
Prior art keywords
permanent magnet
pole
motor
brushless
demagnetization
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN201610811230.5A
Other languages
Chinese (zh)
Other versions
CN106208555A (en
Inventor
刘景林
公超
王晓梅
于昊正
张二阳
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Northwestern Polytechnical University
Original Assignee
Northwestern Polytechnical University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Northwestern Polytechnical University filed Critical Northwestern Polytechnical University
Priority to CN201610811230.5A priority Critical patent/CN106208555B/en
Publication of CN106208555A publication Critical patent/CN106208555A/en
Application granted granted Critical
Publication of CN106208555B publication Critical patent/CN106208555B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K15/00Processes or apparatus specially adapted for manufacturing, assembling, maintaining or repairing of dynamo-electric machines
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K29/00Motors or generators having non-mechanical commutating devices, e.g. discharge tubes or semiconductor devices
    • H02K29/03Motors or generators having non-mechanical commutating devices, e.g. discharge tubes or semiconductor devices with a magnetic circuit specially adapted for avoiding torque ripples or self-starting problems
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K2213/00Specific aspects, not otherwise provided for and not covered by codes H02K2201/00 - H02K2211/00
    • H02K2213/03Machines characterised by numerical values, ranges, mathematical expressions or similar information

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Manufacturing & Machinery (AREA)
  • Permanent Field Magnets Of Synchronous Machinery (AREA)
  • Dc Machiner (AREA)

Abstract

本发明提供了一种内置式无刷直流电机极弧系数的扩展方法,首先,根据内置式无刷直流电机额定工作时每极最大去磁磁势和高温下拐点k处的退磁磁场强度计算永磁体最小边缘厚度;然后,根据最小边缘厚度利用AutoCAD重新设计永磁体形状及尺寸,并测量永磁体边缘间的夹角;最后,根据永磁体边缘间的夹角和极距对应的角度计算无刷直流电机的扩展极弧系数。本发明方法充分利用永磁体槽的结构,通过扩展永磁体边缘,加大永磁体宽度,使得极弧系数得到扩展,既避免了尖角退磁的产生,也避免了极弧系数扩展过程中造成永磁体浪费。利用本发明方法进行极弧系数扩展后,气隙磁密更加接近方波,通过方波控制可以减小电机转矩脉动、振动和噪声。

The invention provides a method for expanding the pole arc coefficient of a built-in brushless DC motor. Firstly, the permanent demagnetization magnetic field strength is calculated according to the maximum demagnetization magnetic potential of each pole and the demagnetization magnetic field strength at the inflection point k at high temperature when the built-in brushless DC motor is in rated operation. The minimum edge thickness of the magnet; then, use AutoCAD to redesign the shape and size of the permanent magnet according to the minimum edge thickness, and measure the angle between the edges of the permanent magnet; finally, calculate the brushless according to the angle between the edges of the permanent magnet and the angle corresponding to the pole pitch Extended pole arc factor for DC motors. The method of the invention makes full use of the structure of the permanent magnet groove, expands the edge of the permanent magnet and increases the width of the permanent magnet, so that the pole arc coefficient is expanded, which not only avoids the generation of sharp demagnetization, but also avoids the permanent magnet in the process of expanding the pole arc coefficient. Magnets are wasted. After using the method of the invention to expand the pole arc coefficient, the air gap magnetic density is closer to the square wave, and the torque ripple, vibration and noise of the motor can be reduced through the square wave control.

Description

一种内置式无刷直流电机极弧系数的扩展方法An Extended Method of Pole Arc Coefficient of Built-in Brushless DC Motor

技术领域technical field

本发明属于电机技术领域,尤其涉及一种内置式无刷直流电机极弧系数的扩展方法。The invention belongs to the technical field of motors, and in particular relates to a method for expanding the pole arc coefficient of a built-in brushless DC motor.

背景技术Background technique

稀土永磁电机具有结构简单、维修方便、运行稳定、性能可靠、功率密度高和调速性能好等优点,已经在风力发电领域、电动汽车领域以及数控机床领域取得了广泛应用;同时,针对永磁电机本体设计与优化的研究也越来越多,研究内容主要包括电机新型结构设计和优化电机参数以达到降低转矩脉动、提高功率因数、获取合理气隙磁密的目标,其中,极弧系数是电机设计的关键参数,直接影响气隙磁密波形,当极弧系数增大时,气隙磁密分布会由正弦波逐渐变为方波,电机反电势方波特性会越好,转矩脉动会减小,电机运行也越平稳,同时也会改善电机电磁振动及噪声,因此,在无刷直流电机设计中,希望极弧系数越大越好。内置式无刷直流电机是无刷直流电机的一种特殊结构,磁钢镶嵌于转子内部,具有更高的可靠性,在内置式无刷直流电机设计中,需要综合考虑电机体积及功率密度,极弧系数的取值会受电机转子大小的限制,在设计过程中若一味追求大的极弧系数,会导致转子隔磁桥部分变小,使得无刷直流电机漏磁增大。Rare earth permanent magnet motors have the advantages of simple structure, convenient maintenance, stable operation, reliable performance, high power density and good speed regulation performance, and have been widely used in the fields of wind power generation, electric vehicles and CNC machine tools; at the same time, for permanent There are more and more studies on the design and optimization of the magneto body. The research content mainly includes the new structure design of the motor and the optimization of the motor parameters to achieve the goals of reducing torque ripple, improving power factor, and obtaining a reasonable air gap flux density. Among them, the pole arc The coefficient is a key parameter in motor design, which directly affects the air-gap magnetic density waveform. When the pole arc coefficient increases, the air-gap magnetic density distribution will gradually change from sine wave to square wave, and the better the square wave characteristics of the motor's back EMF, the better the rotation speed. The torque ripple will be reduced, the motor will run more smoothly, and the electromagnetic vibration and noise of the motor will also be improved. Therefore, in the design of the brushless DC motor, it is hoped that the pole arc coefficient is as large as possible. The built-in brushless DC motor is a special structure of the brushless DC motor. The magnetic steel is embedded in the rotor, which has higher reliability. In the design of the built-in brushless DC motor, it is necessary to comprehensively consider the motor volume and power density. The value of the pole arc coefficient will be limited by the size of the rotor of the motor. If a large pole arc coefficient is blindly pursued in the design process, the part of the magnetic isolation bridge of the rotor will become smaller, which will increase the flux leakage of the brushless DC motor.

为减小漏磁,内置式无刷直流电机永磁体槽的两端会采用三角结构,即永磁体槽尖角,一般设计中,永磁体槽尖角部位不会嵌入永磁体。当所设计的大功率密度内置式无刷直流电机极弧系数比较小时,可以利用永磁体槽尖角对极弧系数进行扩展,方法是在槽尖角位置也填充永磁体以加大永磁体的宽度,但是在该扩展过程中面临一个问题:永磁体槽尖角越接近边缘位置越薄,由于向槽尖角位置填充的永磁体与槽尖角形状一致,当把永磁体嵌入到槽尖角位置或完全填满槽时,永磁体边缘沿充磁方向厚度很小,随着电机工作温度升高,永磁体退磁曲线弯曲,电枢磁场会导致永磁体边缘位置产生不可逆退磁,该现象称为尖角退磁,尖角退磁会导致接近边缘位置的永磁体失效,一味的加大永磁体的宽度,特别是将槽尖角填满时,会造成永磁体因部分失效而产生浪费。因此,极弧系数的扩展会受到尖角退磁的限制。内置式大功率密度无刷直流电机体积小,永磁体的排布空间受到限制,设计过程中极弧系数取不到理想值,需要寻求一种可以避免内置式无刷直流电机永磁体发生尖角退磁的极弧系数扩展方法。In order to reduce magnetic flux leakage, the two ends of the permanent magnet slot of the built-in brushless DC motor will adopt a triangular structure, that is, the sharp corner of the permanent magnet slot. In general design, the permanent magnet will not be embedded in the sharp corner of the permanent magnet slot. When the pole arc coefficient of the designed high power density built-in brushless DC motor is relatively small, the pole arc coefficient can be expanded by using the slot corner of the permanent magnet. The method is to fill the slot corner with permanent magnets to increase the width of the permanent magnet , but there is a problem in the expansion process: the permanent magnet slot tip is thinner as it gets closer to the edge position. Since the permanent magnet filled into the slot tip is consistent with the shape of the slot tip, when the permanent magnet is embedded in the slot tip Or when the groove is completely filled, the thickness of the edge of the permanent magnet along the magnetization direction is very small. As the operating temperature of the motor increases, the demagnetization curve of the permanent magnet bends, and the armature magnetic field will cause irreversible demagnetization at the edge of the permanent magnet. This phenomenon is called sharp Corner demagnetization, sharp corner demagnetization will cause permanent magnets near the edge to fail, and blindly increasing the width of the permanent magnet, especially when filling the sharp corners of the slot, will cause permanent magnets to be wasted due to partial failure. Therefore, the expansion of the pole arc coefficient will be limited by the demagnetization of sharp corners. The built-in high power density brushless DC motor is small in size, and the arrangement space of the permanent magnets is limited. The pole arc coefficient cannot obtain the ideal value during the design process. It is necessary to find a way to avoid the sharp corners of the permanent magnets of the built-in brushless DC motor. Polar arc coefficient expansion method for demagnetization.

发明内容Contents of the invention

要解决的技术问题technical problem to be solved

为弥补在设计功率大、体积小的无刷直流电机过程中无法取得大极弧系数的缺陷,改善方波控制无刷直流电机的性能,并且避免永磁体发生尖角退磁造成浪费,本发明提出一种考虑尖角退磁影响的内置式无刷直流电机极弧系数的扩展方法。In order to make up for the defect that a large pole arc coefficient cannot be obtained in the process of designing a brushless DC motor with large power and small volume, improve the performance of a square wave controlled brushless DC motor, and avoid waste caused by sharp-angle demagnetization of permanent magnets, the present invention proposes An extended method for pole arc coefficients of built-in brushless DC motors considering the effect of demagnetization at sharp corners.

技术方案Technical solutions

一种内置式无刷直流电机极弧系数的扩展方法,其特征在于步骤如下:A method for expanding the pole arc coefficient of a built-in brushless DC motor is characterized in that the steps are as follows:

步骤1:按照h1=Fadm/Hk计算永磁体最小边缘厚度h1,其中,Fadm为内置式无刷直流电机额定工作时每极最大去磁磁势,Hk为温度T时永磁体材料退磁曲线上拐点k处的退磁磁场强度,其中,T≥150℃;Fadm的计算公式为其中,Ia为额定工作电流,WΦ为每相绕组串联匝数,KW为绕组系数,p为极对数;Step 1: Calculate the minimum edge thickness h 1 of the permanent magnet according to h 1 =F adm /H k , where, F adm is the maximum demagnetization magnetic potential per pole when the built-in brushless DC motor is in rated operation, and H k is the permanent magnet at temperature T The demagnetization magnetic field intensity at the inflection point k on the demagnetization curve of the magnet material, where T≥150°C; the calculation formula of F adm is Among them, I a is the rated operating current, W Φ is the number of series turns of each phase winding, K W is the winding coefficient, and p is the number of pole pairs;

步骤2:令扩展后的永磁体边缘厚度等于h1,按照扩展前后永磁体边缘保持平行的原则,利用AutoCAD画出扩展后永磁体形状,并标注永磁体尺寸,同时测量得到扩展后永磁体边缘间的夹角α1,所述的永磁体边缘夹角是每极永磁体两个边缘上端分别与槽的交点A、A’与转子轴心O之间连线的夹角;Step 2: Make the edge thickness of the expanded permanent magnet equal to h 1 . According to the principle of keeping the edges of the permanent magnet parallel before and after the expansion, use AutoCAD to draw the shape of the expanded permanent magnet, mark the size of the permanent magnet, and measure the edge of the expanded permanent magnet at the same time The angle α 1 between the permanent magnet edges is the angle between the upper ends of the two edges of the permanent magnets of each pole and the intersection points A, A' of the slots and the rotor axis O;

步骤3:按照αpmax=α1/β计算得到扩展后内置式无刷直流电机的极弧系数最大值αpmax,则极弧系数的扩展范围是(α/β,αpmax];其中,β是极距对应的角度,α是扩展前永磁体边缘间的夹角。Step 3: According to α pmax = α 1 /β, the maximum value of the pole arc coefficient α pmax of the extended built-in brushless DC motor is obtained, and the expansion range of the pole arc coefficient is (α/β, α pmax ]; where, β is the angle corresponding to the pole pitch, and α is the angle between the edges of the permanent magnet before expansion.

有益效果Beneficial effect

本发明提出的一种内置式无刷直流电机极弧系数的扩展方法,充分利用永磁体槽的结构,通过扩展永磁体边缘,加大永磁体宽度,使得极弧系数得到扩展;利用电机额定工作时每极最大去磁磁势与拐点k处的退磁磁场强度的比值确定永磁体最小边缘厚度,既避免了尖角退磁的产生,也避免了极弧系数扩展过程中造成永磁体浪费。利用本发明方法进行极弧系数扩展后,气隙磁密更加接近方波,通过方波控制可以减小电机转矩脉动、振动和噪声。The method for expanding the pole arc coefficient of a built-in brushless DC motor proposed by the present invention fully utilizes the structure of the permanent magnet slot, expands the edge of the permanent magnet, increases the width of the permanent magnet, and expands the pole arc coefficient; utilizes the rated work of the motor The ratio of the maximum demagnetization magnetic potential of each pole to the demagnetization magnetic field intensity at the inflection point k determines the minimum edge thickness of the permanent magnet, which not only avoids the generation of sharp demagnetization, but also avoids the waste of permanent magnets during the expansion of the pole arc coefficient. After using the method of the invention to expand the pole arc coefficient, the air gap magnetic density is closer to the square wave, and the torque ripple, vibration and noise of the motor can be reduced through the square wave control.

附图说明Description of drawings

图1是本发明的一种内置式无刷直流电机极弧系数扩展方法的计算流程图。Fig. 1 is a calculation flowchart of a pole arc coefficient expansion method of a built-in brushless DC motor according to the present invention.

图2为钕铁硼35SH在150℃时退磁曲线。Figure 2 is the demagnetization curve of NdFeB 35SH at 150°C.

图3为内置式无刷直流电机极弧系数扩展前后转子示意图。Figure 3 is a schematic diagram of the rotor before and after the expansion of the pole arc coefficient of the built-in brushless DC motor.

具体实施方式Detailed ways

下面结合附图和实施例对本发明进一步说明,本发明包括但不仅限于下述实施例。The present invention will be further described below in conjunction with the accompanying drawings and embodiments, and the present invention includes but not limited to the following embodiments.

由于内置式无刷直流电机极弧系数大小与转子上永磁体的空间分布有关,永磁体宽度越宽,电机极弧系数越大。若将槽尖角部分填充永磁体可以扩展永磁体的宽度,极弧系数随之加大,使得无刷直流电机气隙磁密更加接近方波,方波控制该无刷直流电机转矩脉动和噪声会减小。然而,当电机工作温度高于某值时,绕组产生的退磁磁场超过一定值后,永磁体退磁曲线会急剧下降,新的恢复曲线不再与退磁曲线重合,产生不可逆退磁,退磁后的永磁体向外提供的磁密急剧减小,重复工作甚至导致永磁体完全失磁,所以在永磁体向槽尖角扩展时需要校核最小厚度,避免发生尖角退磁,同时可以防止永磁体浪费。Since the pole arc coefficient of the built-in brushless DC motor is related to the spatial distribution of the permanent magnets on the rotor, the wider the permanent magnet width, the larger the pole arc coefficient of the motor. If the slot corners are filled with permanent magnets, the width of the permanent magnets can be expanded, and the pole arc coefficient will increase accordingly, making the air gap magnetic density of the brushless DC motor closer to the square wave. The square wave controls the torque ripple of the brushless DC motor and Noise will be reduced. However, when the working temperature of the motor is higher than a certain value, after the demagnetization magnetic field generated by the winding exceeds a certain value, the demagnetization curve of the permanent magnet will drop sharply, and the new recovery curve will no longer coincide with the demagnetization curve, resulting in irreversible demagnetization, and the permanent magnet after demagnetization The magnetic density provided to the outside decreases sharply, and repeated work even leads to the complete loss of magnetism of the permanent magnet. Therefore, when the permanent magnet expands to the sharp corner of the slot, it is necessary to check the minimum thickness to avoid demagnetization at the sharp corner and prevent waste of the permanent magnet.

基于上述思想,如图1所示,本发明的考虑尖角退磁影响的永磁电机极弧系数扩展方法具体过程如下:Based on the above thought, as shown in Figure 1, the specific process of the permanent magnet motor pole arc coefficient expansion method considering the influence of sharp angle demagnetization of the present invention is as follows:

1)确定永磁体退磁曲线拐点k处的退磁磁场强度Hk 1) Determine the demagnetization magnetic field strength H k at the inflection point k of the permanent magnet demagnetization curve

尖角退磁发生在高温条件下,长时间工作的大功率密度永磁电机内部温度在100℃以上,本实施例电机工作温度约为150℃,选择150℃钕铁硼35SH退磁曲线拐点k处的磁场强度来计算的永磁体最小边缘厚度,如图2所示,拐点k处退磁磁场强度大小为Hk=487000A/m;Sharp-angle demagnetization occurs under high temperature conditions. The internal temperature of the high-power-density permanent magnet motor that works for a long time is above 100°C. The operating temperature of the motor in this example is about 150°C. The minimum edge thickness of the permanent magnet calculated based on the magnetic field strength, as shown in Figure 2, the demagnetization magnetic field strength at the inflection point k is Hk =487000A/m;

2)确定无刷直流电机额定工作时每极最大去磁磁势Fadm 2) Determine the maximum demagnetization magnetic potential F adm per pole when the brushless DC motor is rated to work

电机长时间处于额定工作状态时温度升高,之后电机绕组电流产生的退磁磁场会导致永磁体发生不可逆退磁,所以,要估算永磁体的最小厚度需要首先确定电机额定工作时每极最大去磁磁势,计算公式是其中,Ia为额定工作电流,WΦ为每相绕组串联匝数,KW为绕组系数,p为极对数。本实施例的内置式无刷直流电机转子示意图如图3所示,其额定电流Ia=50A,每相绕组串联匝数WΦ=42,绕组系数KW=0.96,极对数p=3,则可计算得到每极最大去磁磁势为Fadm=581.9A。When the motor is in the rated working state for a long time, the temperature rises, and then the demagnetization magnetic field generated by the motor winding current will cause irreversible demagnetization of the permanent magnet. Therefore, to estimate the minimum thickness of the permanent magnet, it is necessary to first determine the maximum demagnetization of each pole when the motor is rated. Potential, the calculation formula is Among them, I a is the rated operating current, W Φ is the number of series turns of each phase winding, K W is the winding coefficient, and p is the number of pole pairs. The schematic diagram of the built-in brushless DC motor rotor of this embodiment is shown in Figure 3, its rated current I a = 50A, the number of series turns of each phase winding W Φ = 42, the winding coefficient K W = 0.96, and the number of pole pairs p = 3 , then the maximum demagnetization magnetic potential per pole can be calculated as F adm =581.9A.

3)计算永磁体最小边缘厚度hmin 3) Calculate the minimum edge thickness h min of the permanent magnet

根据磁势等于距离乘磁场强度可得永磁体最小边缘厚度等于每极最大去磁磁势Fadm除以磁场强度Hk,计算公式为hmin=Fadm/Hk,本实施例最小厚度为hmin=1.19mm。According to the magnetic potential is equal to the distance multiplied by the magnetic field strength, the minimum edge thickness of the permanent magnet is equal to the maximum demagnetization magnetic potential F adm divided by the magnetic field strength H k , the calculation formula is h min =F adm /H k , the minimum thickness of the present embodiment is hmin = 1.19 mm.

4)重新设计永磁体4) Redesign the permanent magnet

永磁体槽的形状与尺寸由预取极弧系数αp和隔磁桥宽度c决定,如图3所示,本实施中永磁体边缘顶点与A点重合,永磁体形状和永磁体槽一致,槽边缘位置形成槽尖角,该位置有一部分没有永磁体填充。其中,αp=α/β,α是永磁体边缘间的夹角,即每极永磁体两个边缘上端分别与槽的交点A、A’与转子轴心O之间连线的夹角,β是极距对应的角度,本实施例中预取极弧系数αp为0.83,永磁体边缘间的夹角α=50°,极距对应的角度β=60°。The shape and size of the permanent magnet slot are determined by the prefetch pole arc coefficient α p and the width c of the magnetic isolation bridge. The slot edge position forms the slot tip, and a part of this position is not filled with a permanent magnet. Among them, α p = α/β, α is the angle between the edges of the permanent magnet, that is, the angle between the upper ends of the two edges of the permanent magnet of each pole and the intersection points A and A' of the groove and the rotor axis O, respectively, β is the angle corresponding to the pole pitch. In this embodiment, the prefetched pole arc coefficient α p is 0.83, the angle between the edges of the permanent magnets is α=50°, and the angle β=60° corresponding to the pole pitch.

为避免尖角退磁的发生,以永磁体最小边缘厚度hmin为永磁体加宽的边界条件,即令扩展后永磁体的边缘厚度h1=hmin,依托永磁体槽型结构,利用AutoCAD直接在槽尖角内画出永磁体边缘,按照扩展前后永磁体边缘保持平行的原则,永磁体边缘仍与槽边缘AB垂直,即h1//h,如图3所示,扩展后得到的新永磁体是原永磁体和永磁体扩展部分的和,该过程永磁体的外形发生了改变,利用AutoCAD可直接测量永磁体各部分尺寸,并进行标注。In order to avoid the occurrence of sharp demagnetization, the minimum edge thickness h min of the permanent magnet is used as the boundary condition for the widening of the permanent magnet, that is, the edge thickness of the permanent magnet after expansion is h 1 =h min , relying on the groove structure of the permanent magnet, using AutoCAD to directly Draw the edge of the permanent magnet in the sharp corner of the slot. According to the principle that the edge of the permanent magnet remains parallel before and after expansion, the edge of the permanent magnet is still perpendicular to the edge AB of the slot, that is, h 1 //h. As shown in Figure 3, the new permanent magnet obtained after expansion The magnet is the sum of the original permanent magnet and the extended part of the permanent magnet. During this process, the shape of the permanent magnet has changed. Using AutoCAD, the size of each part of the permanent magnet can be directly measured and marked.

永磁体宽度扩展后,永磁体边缘间的夹角变大,可通过AutoCAD测量得到:新永磁体上端边缘与槽产生新的交点C1、C2,从转子轴心O向这两点作辅助线,测量两条线段之间夹角,即扩展后永磁体边缘间的夹角α1=55.8°。After the width of the permanent magnet is expanded, the angle between the edges of the permanent magnet becomes larger, which can be measured by AutoCAD: new intersection points C 1 and C 2 are generated between the upper edge of the new permanent magnet and the slot, and are assisted from the rotor axis O to these two points line, measuring the angle between two line segments, that is, the angle α 1 between the edges of the expanded permanent magnet = 55.8°.

5)计算扩展后内置式无刷直流电机的极弧系数αpmax 5) Calculate the pole arc coefficient α pmax of the extended built-in brushless DC motor

按αpmax=α1/β扩展后的极弧系数αpmax,本实施例扩展后的极弧系数为αpmax=0.93,可以看出较预取极弧系数增大很多。需要说明的是:αpmax是能避免尖角退磁的最大极弧系数,优化过程中取(α/β,αpmax]之间任何值都可以避免尖角退磁现象发生。According to α pmax1 /β expanded polar arc coefficient α pmax , the expanded polar arc coefficient in this embodiment is α pmax =0.93, which is much larger than the prefetched polar arc coefficient. It should be noted that α pmax is the maximum pole arc coefficient that can avoid sharp-angle demagnetization, and any value between (α/β, α pmax ] during optimization can avoid sharp-angle demagnetization.

Claims (1)

1.一种内置式无刷直流电机极弧系数的扩展方法,其特征在于步骤如下:1. A method for expanding the pole arc coefficient of a built-in brushless DC motor, characterized in that the steps are as follows: 步骤1:按照h1=Fadm/Hk计算永磁体最小边缘厚度h1,其中,Fadm为内置式无刷直流电机额定工作时每极最大去磁磁势,Hk为温度T时永磁体材料退磁曲线上拐点k处的退磁磁场强度,其中,T≥150℃;Fadm的计算公式为其中,Ia为额定工作电流,WΦ为每相绕组串联匝数,KW为绕组系数,p为极对数;Step 1: Calculate the minimum edge thickness h 1 of the permanent magnet according to h 1 =F adm /H k , where, F adm is the maximum demagnetization magnetic potential per pole when the built-in brushless DC motor is in rated operation, and H k is the permanent magnet at temperature T The demagnetization magnetic field intensity at the inflection point k on the demagnetization curve of the magnet material, where T≥150°C; the calculation formula of F adm is Among them, I a is the rated operating current, W Φ is the number of series turns of each phase winding, K W is the winding coefficient, and p is the number of pole pairs; 步骤2:令扩展后的永磁体边缘厚度等于h1,按照扩展前后永磁体边缘保持平行的原则,利用AutoCAD画出扩展后永磁体形状,并标注永磁体尺寸,同时测量得到扩展后永磁体边缘间的夹角α1,所述的永磁体边缘夹角是每极永磁体两个边缘上端分别与槽的交点A、A’与转子轴心O之间连线的夹角;Step 2: Make the edge thickness of the expanded permanent magnet equal to h 1 . According to the principle of keeping the edges of the permanent magnet parallel before and after the expansion, use AutoCAD to draw the shape of the expanded permanent magnet, mark the size of the permanent magnet, and measure the edge of the expanded permanent magnet at the same time The angle α 1 between the permanent magnet edges is the angle between the upper ends of the two edges of the permanent magnets of each pole and the intersection points A, A' of the slots and the rotor axis O; 步骤3:按照αpmax=α1/β计算得到扩展后内置式无刷直流电机的极弧系数最大值αpmax,则极弧系数的扩展范围是(α/β,αpmax];其中,β是极距对应的角度,α是扩展前永磁体边缘间的夹角。Step 3: According to α pmax = α 1 /β, the maximum value of the pole arc coefficient α pmax of the extended built-in brushless DC motor is obtained, and the expansion range of the pole arc coefficient is (α/β, α pmax ]; where, β is the angle corresponding to the pole pitch, and α is the angle between the edges of the permanent magnet before expansion.
CN201610811230.5A 2016-09-09 2016-09-09 A kind of extended method of built-in brshless DC motor pole embrace Active CN106208555B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610811230.5A CN106208555B (en) 2016-09-09 2016-09-09 A kind of extended method of built-in brshless DC motor pole embrace

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610811230.5A CN106208555B (en) 2016-09-09 2016-09-09 A kind of extended method of built-in brshless DC motor pole embrace

Publications (2)

Publication Number Publication Date
CN106208555A CN106208555A (en) 2016-12-07
CN106208555B true CN106208555B (en) 2018-08-07

Family

ID=58066846

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610811230.5A Active CN106208555B (en) 2016-09-09 2016-09-09 A kind of extended method of built-in brshless DC motor pole embrace

Country Status (1)

Country Link
CN (1) CN106208555B (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107276355A (en) * 2017-07-27 2017-10-20 西安思坦科技有限公司 A kind of permanent magnet low-speed directly drives synchronous motor
CN114047441B (en) * 2021-11-09 2024-04-30 常州隆耐智能装备有限公司 A permanent magnet synchronous motor integrated drive control system and method

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3333359B2 (en) * 1995-09-22 2002-10-15 三菱電機株式会社 Permanent magnet type motor
CN104158458B (en) * 2014-07-24 2017-01-18 天津大学 Magnetic field analytic calculating method for surface-mounted permanent magnet motor with tilted trough structure

Also Published As

Publication number Publication date
CN106208555A (en) 2016-12-07

Similar Documents

Publication Publication Date Title
Xu et al. Flux-leakage design principle and multiple-operating conditions modeling of flux leakage controllable PM machine considering driving cycles
Kim et al. Optimization methods of torque density for developing the neodymium free SPOKE-type BLDC motor
Shen et al. A coaxial magnetic gear with consequent-pole rotors
CN105356679B (en) The design method of magnetic flux switching external rotor electric machine based on electric heating bidirectional couple
CN112257231B (en) Permanent magnet motor analysis method and system considering nonlinear characteristics of silicon steel sheet and application
CN105179289A (en) Method for controlling variable-speed fan system
CN108566004A (en) Widen the rotor structure Robust-Design of the internal permanent magnet synchronous motor range of speeds
CN109672304A (en) A kind of moving-magnetic type permanent magnetic linear synchronous motor design method inhibited based on longitudinal end effect
Hao et al. Analysis of cogging torque reduction techniques in axial-field flux-switching permanent-magnet machine
CN106208555B (en) A kind of extended method of built-in brshless DC motor pole embrace
Bouloukza et al. Electromagnetic design of a new radial flux permanent magnet motor
CN103929033A (en) A permanent magnet synchronous motor rotor structure with bow-shaped permanent magnets
Wang et al. Interior permanent magnet synchronous machines with composed T-shaped notching rotor
CN103915926B (en) Rotor structure for permanent magnet synchronous motor with triangular-step-shaped permanent magnets
Infantraj et al. Investigation of various laminating materials for interior permanent magnet brushless DC motor for cooling fan application
Drancă et al. Thermal and demagnetization analysis of an axial-flux permanent magnet synchronous machine
Weili et al. Loss calculation and thermal simulation analysis of high-speed PM synchronous generators with rotor topology
CN105356804B (en) Improve synchronous magnetic resistance motor salient pole than method
Huang et al. Design and thermal analysis on high torque low speed fractional-slot concentrated windings in-wheel traction motor
Jing et al. Analysis and reduction of cogging torque of line-start permanent magnet motors
CN107729628B (en) A Nonlinear Inductance Modeling Method for Three-Phase Electrically Excited Doubly Salient Motors
CN117060670A (en) Effective method for inhibiting eddy current loss of permanent magnet of spoke type magnetic field modulation motor
Zhou et al. A current coordinated optimal control strategy for doubly salient electromagnetic machine
Wang et al. The impact of excitation voltage fluctuation on phase current of switched reluctance generator
Yujie et al. Design and finite element analysis of outer-rotor-type switched reluctance generator in wind power generation

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant