CN107203669A - A kind of Reverse optimization design method of MR damper - Google Patents

A kind of Reverse optimization design method of MR damper Download PDF

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CN107203669A
CN107203669A CN201710411418.5A CN201710411418A CN107203669A CN 107203669 A CN107203669 A CN 107203669A CN 201710411418 A CN201710411418 A CN 201710411418A CN 107203669 A CN107203669 A CN 107203669A
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徐赵东
王成
赵玉亮
苗安男
杨昀
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Southeast University
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Abstract

本发明公开了一种磁流变阻尼器的反向优化设计方法,该方法通过选定所需的最大阻尼力和可调系数,将几何设计和磁路设计统一起来进行反向优化设计,直到磁流变阻尼器在相对小的尺寸下满足所需的最大阻尼力和可调系数;其中,几何设计利用MATLAB仿真软件计算几何设计目标值,磁路设计利用ANSYS有限元仿真计算磁路设计目标值。本发明的反向优化设计方法既满足了磁路设计中空间磁场强度解的精准度,又充分考虑几何设计和磁路设计之间的相互关联性,有效避免了过早出现磁饱和现象或磁路材料的浪费;该方法可操作性强,为磁流变阻尼器的设计提供了理论指导,便于其工程应用和推广。

The invention discloses a reverse optimization design method of a magneto-rheological damper. By selecting the required maximum damping force and adjustable coefficient, the method unifies the geometric design and the magnetic circuit design for reverse optimization design until The magnetorheological damper meets the required maximum damping force and adjustable coefficient in a relatively small size; among them, the geometric design uses MATLAB simulation software to calculate the geometric design target value, and the magnetic circuit design uses ANSYS finite element simulation to calculate the magnetic circuit design target value. The reverse optimization design method of the present invention not only satisfies the accuracy of the spatial magnetic field strength solution in the magnetic circuit design, but also fully considers the interrelationship between the geometric design and the magnetic circuit design, effectively avoiding premature magnetic saturation or magnetic The waste of road materials; this method has strong operability, and provides theoretical guidance for the design of magnetorheological dampers, which is convenient for its engineering application and promotion.

Description

一种磁流变阻尼器的反向优化设计方法A Reverse Optimal Design Method for Magnetorheological Damper

技术领域technical field

本发明涉及一种可用于智能控制领域的磁流变阻尼器的反向优化设计方法。The invention relates to a reverse optimization design method of a magneto-rheological damper that can be used in the field of intelligent control.

背景技术Background technique

近年来,我国对工程结构采用振动控制技术来减轻地震和强风灾害的研究越来越多,具体的技术手段也日益增多,并被广泛应用于实际工程。结构振动控制是指通过对结构附设控制构件和控制装置,当结构振动时被动或主动的给结构施加一组控制力,减小或抑制结构的动力反应,以满足结构的安全性、使用性和舒适度的要求。In recent years, there have been more and more researches on the use of vibration control technology for engineering structures to mitigate earthquake and strong wind disasters, and more and more specific technical means have been widely used in practical projects. Structural vibration control refers to attaching control components and control devices to the structure, passively or actively exerting a set of control forces on the structure when the structure vibrates, reducing or inhibiting the dynamic response of the structure, so as to meet the safety, usability and safety of the structure. comfort requirements.

磁流变阻尼器是结构振动控制中半主动控制装置的代表,具有耗能小、出力大、响应速度快、阻尼力连续可调等优点,可实现较好的振动控制效果。显然,方便有效的磁流变阻尼器设计方法对其制作和工程应用而言至关重要。目前,设计磁流变阻尼器的基本思路大致为:首先依据阻尼器最大阻尼力设计阻尼器几何参数;然后按照几何设计中选定的最大剪切屈服强度所需的磁感应强度和几何设计确定的参数尺寸,利用磁路欧姆定律进行磁路设计。此设计思路虽然切实可行,但是设计过程是将几何设计与磁路设计分开独立进行的,未能充分考虑两者之间的相互关联。针对以上问题,有学者引入磁路优化把磁路设计与几何设计融为一体,提出了一种简化的剪切阀式磁流变阻尼器设计方法;但是其磁路部分仍是采用磁路欧姆定律得到的计算公式进行设计的,然而铁磁体组合结构较为复杂,所以很难得到通电后空间磁场强度的精准解析解。有学者利用有限元精准仿真磁场,以最大阻尼力和可调系数为优化目标,利用多目标遗传算法,对磁流变阻尼器进行了优化设计;但其目标函数是使最大阻尼力最大和使可调系数最大,而实际工程减振设计中通常是在给定所需最大阻尼力和可调系数的情况下进行反向参数优化设计,使得阻尼器在较小的尺寸下满足设计要求。因此必须在现有磁流变阻尼器设计方法的基础上寻求创新。Magneto-rheological damper is a representative of semi-active control devices in structural vibration control. It has the advantages of low energy consumption, large output, fast response speed, continuously adjustable damping force, etc., and can achieve better vibration control effects. Obviously, a convenient and effective design method for magnetorheological dampers is very important for its fabrication and engineering applications. At present, the basic idea of designing a magneto-rheological damper is roughly as follows: firstly, the geometric parameters of the damper are designed according to the maximum damping force of the damper; Parameter size, using the magnetic circuit Ohm's law for magnetic circuit design. Although this design idea is feasible, the design process separates the geometric design from the magnetic circuit design and fails to fully consider the interrelationship between the two. In response to the above problems, some scholars introduced magnetic circuit optimization to integrate magnetic circuit design and geometric design, and proposed a simplified design method for shear valve magneto-rheological dampers; however, the magnetic circuit part still uses the magnetic circuit ohm However, the combined structure of ferromagnets is relatively complex, so it is difficult to obtain an accurate analytical solution of the spatial magnetic field strength after electrification. Some scholars use finite elements to accurately simulate the magnetic field, take the maximum damping force and adjustable coefficient as the optimization goal, and use the multi-objective genetic algorithm to optimize the design of the magnetorheological damper; but the objective function is to maximize the maximum damping force and make the The adjustable coefficient is the largest, and in the actual engineering vibration reduction design, the reverse parameter optimization design is usually carried out under the condition of given the required maximum damping force and adjustable coefficient, so that the damper can meet the design requirements in a smaller size. Therefore, innovation must be sought on the basis of the existing design methods of magneto-rheological dampers.

发明内容Contents of the invention

发明目的:本发明所要解决的技术问题是提供一种磁流变阻尼器的反向优化设计方法,使得阻尼器在较小尺寸下能够满足给定的最大阻尼力和可调系数要求。Purpose of the invention: The technical problem to be solved by the present invention is to provide a reverse optimization design method of a magneto-rheological damper, so that the damper can meet the given maximum damping force and adjustable coefficient requirements in a smaller size.

发明内容:为解决上述技术问题,本发明所采用的技术手段为:Summary of the invention: In order to solve the above technical problems, the technical means adopted in the present invention are:

一种磁流变阻尼器的反向优化设计方法,该方法通过确定所需的最大阻尼力和可调系数,将几何设计和磁路设计统一起来进行反向优化设计,直到磁流变阻尼器在相对小的尺寸下满足所需的最大阻尼力和可调系数;其中,几何设计利用MATLAB仿真软件计算几何设计目标值,磁路设计利用ANSYS有限元仿真计算磁路设计目标值。A reverse optimization design method of magnetorheological damper, the method unifies geometric design and magnetic circuit design by determining the required maximum damping force and adjustable coefficient, and carries out reverse optimization design until the magnetorheological damper The required maximum damping force and adjustable coefficient are met under a relatively small size; among them, the geometric design uses MATLAB simulation software to calculate the geometric design target value, and the magnetic circuit design uses ANSYS finite element simulation to calculate the magnetic circuit design target value.

本发明方法具体包括如下步骤:The inventive method specifically comprises the steps:

步骤1,选定磁流变阻尼器的设计目标值:最大阻尼力U*和可调系数β0Step 1, select the design target value of the magneto-rheological damper: maximum damping force U * and adjustable coefficient β 0 ;

步骤2,依据实际振动情况确定所需阻尼器活塞杆的最大速度再结合选取的磁流变液和磁路材料确定磁流变液工作点对应的最大剪切屈服强度τy,和零场粘度η;Step 2. Determine the maximum speed of the required damper piston rod according to the actual vibration situation Then combine the selected magnetorheological fluid and magnetic circuit material to determine the maximum shear yield strength τ y corresponding to the working point of the magnetorheological fluid, and the zero-field viscosity η;

步骤3,根据步骤1确定的最大阻尼力U*,按照机械设计规范和材料力学特性计算所需活塞杆直径d和外缸筒厚度t的强度限值;Step 3, according to the maximum damping force U * determined in step 1, calculate the required piston rod diameter d and the strength limit of the outer cylinder thickness t according to the mechanical design specifications and material mechanical properties;

步骤4,确定各个材料的导磁特性并根据步骤2中选定的最大剪切屈服强度τy查找磁路工作间隙处所需磁感应强度B0Step 4, determine the magnetic permeability characteristics of each material and find the required magnetic induction intensity B 0 at the working gap of the magnetic circuit according to the maximum shear yield strength τ y selected in step 2;

步骤5,根据步骤3确定的活塞杆直径d的强度限值进行几何设计;Step 5, perform geometric design according to the strength limit value of the piston rod diameter d determined in step 3;

步骤6,根据步骤3确定的外缸筒厚度t的强度限值和步骤4确定的磁路工作间隙处所需磁感应强度B0进行磁路设计;Step 6, carry out magnetic circuit design according to the strength limit value of the outer cylinder barrel thickness t determined in step 3 and the required magnetic induction intensity B at the working gap of the magnetic circuit determined in step 4;

步骤7,判断设计的几何参数和磁路参数是否满足要求,如果不满足要求则重复步骤5~6,直到几何参数和磁路参数达到最小尺寸且满足步骤1中确定的最大设计阻尼力U*和可调系数β0的要求。Step 7. Determine whether the designed geometric parameters and magnetic circuit parameters meet the requirements. If not, repeat steps 5 to 6 until the geometric parameters and magnetic circuit parameters reach the minimum size and meet the maximum design damping force U * determined in step 1. And adjustable coefficient β 0 requirements.

其中,步骤5中,所述几何设计的设计步骤包括:(1)初步选取几何尺寸参数活塞直径D、活塞杆直径d、工作间隙宽度h和活塞有效长度L;(2)利用MATLAB仿真软件计算当前选取的初始参数下得到的最大阻尼力和可调系数;(3)并将(2)得到的数值与设计目标值比较,若不满足设计要求,重新选取几何尺寸参数,再重复(1)~(3),直到仿真计算得到的数值满足设计要求为止;(4)当仿真计算得到的数值满足设计要求后,再判断设定的初始参数是否可以进一步减小,如果可以则重新选取较小值重复步骤(1)~(4),否则选取设定的参数为设计结果。Wherein, in step 5, the design steps of the geometric design include: (1) preliminary selection of geometric dimension parameters piston diameter D, piston rod diameter d, working gap width h and piston effective length L; (2) utilizing MATLAB simulation software to calculate The maximum damping force and adjustable coefficient obtained under the currently selected initial parameters; (3) compare the value obtained in (2) with the design target value, if the design requirements are not met, re-select the geometric size parameters, and repeat (1) ~(3), until the value obtained by simulation calculation meets the design requirements; (4) When the value obtained by simulation calculation meets the design requirements, then judge whether the set initial parameters can be further reduced, and if so, select a smaller value value, repeat steps (1) to (4), otherwise select the set parameters as the design result.

其中,步骤6中,所述磁路设计的设计步骤包括:(1)根据几何设计结果,初步选取定线圈匝数N、外缸筒厚度t、挖槽长度a与宽度b;(2)利用磁路ANSYS有限元仿真计算工作间隙处平均磁感应强度(3)判断挖槽长度a与宽度b是否小于限值,如果满足则进行下一步,否则重新进行几何设计并进行步骤(1)~(3);(4)判断步骤(2)中工作间隙处平均磁感应强度是否大于或等于选定的磁路工作间隙处磁感应强度B0,如果满足,则进行下一步,否则重复步骤(1)~(4);(5)判断设定的初始参数是否可以进一步减小,如果可以则重新选取较小值重复步骤(1)~(5),否则选取设定的参数为设计结果。Wherein, in step 6, the design steps of the magnetic circuit design include: (1) according to the geometric design results, preliminarily select the number of turns N of the fixed coil, the thickness t of the outer cylinder, the length a and the width b of the groove; (2) use Magnetic circuit ANSYS finite element simulation to calculate the average magnetic induction intensity at the working gap (3) Judging whether the length a and width b of the excavation are less than the limit value, if they are satisfied, go to the next step, otherwise, re-design the geometry and go to steps (1)~(3); (4) Judging the working gap in step (2) average magnetic induction Whether it is greater than or equal to the magnetic induction intensity B 0 at the working gap of the selected magnetic circuit, if it is satisfied, proceed to the next step, otherwise repeat steps (1)~(4); (5) judge whether the set initial parameters can be further reduced , if possible, select a smaller value and repeat steps (1) to (5), otherwise, select the set parameter as the design result.

其中,考虑挖槽长度a与宽度b的力学特性要求,挖槽长度a的限值取活塞头长度的四分之一,挖槽宽度b的限值取活塞头直径与活塞杆直径差值的二分之一。Among them, considering the mechanical characteristics requirements of the length a and width b of the groove, the limit value of the length a of the groove is taken as a quarter of the length of the piston head, and the limit value of the width b of the groove is taken as the difference between the diameter of the piston head and the diameter of the piston rod Half.

其中,所述ANSYS有限元仿真的具体分析过程为:(1)选用二维静态分析类型,单元选用二维8节点四边形实体单元Plane53;(2)根据已知材料的导磁特性分别建立活塞、缸筒、间隙磁流变液、线圈、空气和密封环氧树脂部分的有限元模型;(3)在模型外边界线施加磁通量平行的边界条件,划分网格;(4)以电流密度的形式施加激励,对该模型进行静态求解;(5)进入后处理,查看磁场强度数据,进行工作间隙处平均磁感应强度的计算。Wherein, the specific analysis process of the ANSYS finite element simulation is: (1) select the two-dimensional static analysis type, and the unit selects the two-dimensional 8-node quadrilateral solid element Plane53; (2) establish the piston, The finite element model of the cylinder, gap magnetorheological fluid, coil, air and sealing epoxy resin; (3) apply the boundary condition parallel to the magnetic flux on the outer boundary line of the model, and divide the grid; (4) apply it in the form of current density Excitation, statically solve the model; (5) enter the post-processing, check the magnetic field strength data, and carry out the average magnetic induction intensity at the working gap calculation.

其中,所述最大阻尼力和可调系数的计算公式分别为:Wherein, the calculation formulas of the maximum damping force and the adjustable coefficient are respectively:

FMRD,max=Fτ+Fη+Fp0F MRD, max = F τ + F η + F p0 ;

式中, p0=1.2Mpa。In the formula, p 0 =1.2 MPa.

相比于现有技术,本发明技术方案具有的有益效果为:Compared with the prior art, the technical solution of the present invention has the beneficial effects of:

首先,本发明方法通过统一几何设计和磁路设计对磁流变阻尼器进行反向优化设计,使得阻尼器在较小尺寸下能够满足给定的最大阻尼力和可调系数要求;同时,利用MATLAB和ANSYS分别仿真计算几何设计和磁路设计中的目标值,反复试算,综合比较,满足要求为止,这样既满足了磁路设计中空间磁场强度解的精准度,又充分考虑几何设计和磁路设计之间的相互关联性,有效避免了过早出现磁饱和现象或磁路材料的浪费;其次,设计流程上适应了实际工程结构减振设计中已知最大阻尼力和可调系数来反向设计磁流变阻尼器的流程需求,达到了工程上的经济性;最后,本发明方法可操作性强,为磁流变阻尼器的设计提供了理论指导,便于其工程应用和推广。Firstly, the method of the present invention performs reverse optimization design on the magneto-rheological damper through unified geometric design and magnetic circuit design, so that the damper can meet the given maximum damping force and adjustable coefficient requirements in a smaller size; at the same time, using MATLAB and ANSYS respectively simulate and calculate the target values in the geometric design and magnetic circuit design, repeated trial calculations, and comprehensive comparisons until the requirements are met. This not only meets the accuracy of the space magnetic field strength solution in the magnetic circuit design, but also fully considers the geometric design and The interrelationship between magnetic circuit designs effectively avoids premature magnetic saturation or waste of magnetic circuit materials; secondly, the design process adapts to the known maximum damping force and adjustable coefficient in the actual engineering structure vibration reduction design. The reverse design of the flow requirements of the magneto-rheological damper achieves engineering economy; finally, the method of the present invention has strong operability, provides theoretical guidance for the design of the magnetorheological damper, and facilitates its engineering application and promotion.

附图说明Description of drawings

图1为本发明磁流变阻尼器的反向优化设计方法的流程框图;Fig. 1 is the flowchart of the reverse optimal design method of magneto-rheological damper of the present invention;

图2为磁路材料的B-H曲线;Figure 2 is the B-H curve of the magnetic circuit material;

图3为磁流变液零场粘度-速度曲线;Fig. 3 is the zero-field viscosity-velocity curve of magnetorheological fluid;

图4为磁流变液B-H曲线;Fig. 4 is the B-H curve of magnetorheological fluid;

图5为磁流变液τy-B曲线。Fig. 5 is the τ y -B curve of the magnetorheological fluid.

具体实施方式detailed description

根据下述实施例,可以更好地理解本发明。然而,本领域的技术人员容易理解,实施例所描述的内容仅用于说明本发明,而不应当也不会限制权利要求书中所详细描述的本发明。The present invention can be better understood from the following examples. However, those skilled in the art can easily understand that the content described in the embodiments is only for illustrating the present invention, and should not and will not limit the present invention described in the claims.

如图1所示,本发明磁流变阻尼器的反向优化设计方法,在给定所需的最大阻尼力和可调系数的情况下,将几何设计和磁路设计统一起来进行优化设计,以使得磁流变阻尼器在较小的尺寸下能够满足所需的最大阻尼力和可调系数。As shown in Figure 1, the reverse optimal design method of the magneto-rheological damper of the present invention, under the condition of given the required maximum damping force and adjustable coefficient, unifies the geometric design and the magnetic circuit design to optimize the design, So that the magneto-rheological damper can meet the required maximum damping force and adjustable coefficient in a smaller size.

结合土木工程结构减震的特点和统一优化设计过程,本实施例设计一台阻尼力1.5KN的磁流变阻尼器,即最大阻尼力U*=1.5KN,阻尼器工作最大速度为25mm/s,可调系数β0取1.2。活塞及活塞杆采用DT4电工纯铁,并且将活塞及活塞杆连为一体,其余构件均采用45#钢,图2为两者的B-H曲线。漆包线选择直径为1mm的铜导线。有限元模拟时漆包线、空气、环氧树脂的相对磁导率均取1。磁流变液可以是市场上的磁流变液,但是优选本课题组研制的CB22型磁流变液,其中,图3为磁流变液在25℃下的零场粘度-速度关系曲线,图4为磁流变液的B-H曲线,图5为磁流变液的τy-B曲线。测到磁感应强度B=300mT,取磁流变液τy-B曲线中磁感应强度为0.3T时的点为磁流变液的工作点,所以磁路设计中工作间隙处磁感应强度B0为0.3T,此时对应的最大剪切屈服强度τy为4.64KPa。根据图3拟合零场粘度-速度的关系曲线计算阻尼器工作最大速度25mm/s下零场粘度η为1.45pa.s。考虑到磁饱和电流太小,则电流的调节范围较小,磁饱和电流太大,则阻尼器功率较大,易发烫,综合考虑选定Imax为1.5A。依据机械设计规范、材料力学特性和阻尼器受力情况计算活塞杆直径d的强度限值为10.23mm(活塞杆开孔4mm),外缸筒厚度t的强度限值为3.05mm。Combining the characteristics of shock absorption of civil engineering structures and the unified optimization design process, this embodiment designs a magneto-rheological damper with a damping force of 1.5KN, that is, the maximum damping force U * = 1.5KN, and the maximum working speed of the damper is 25mm/s, and the adjustable coefficient β 0 is 1.2. The piston and piston rod are made of DT 4 electrical pure iron, and the piston and piston rod are connected as a whole, and the rest of the components are made of 45 # steel. Figure 2 shows the BH curve of the two. The enameled wire is a copper wire with a diameter of 1mm. The relative magnetic permeability of enameled wire, air and epoxy resin is taken as 1 during finite element simulation. The magnetorheological fluid can be the magnetorheological fluid on the market, but the CB22 magnetorheological fluid developed by our research group is preferred. Among them, Figure 3 is the zero-field viscosity-velocity curve of the magnetorheological fluid at 25°C. Fig. 4 is the BH curve of the magnetorheological fluid, and Fig. 5 is the τ y -B curve of the magnetorheological fluid. The magnetic induction intensity B=300mT is measured, and the point in the magnetorheological fluid τ y -B curve when the magnetic induction intensity is 0.3T is the working point of the magnetorheological fluid, so the magnetic induction intensity B 0 at the working gap in the magnetic circuit design is 0.3 T, the corresponding maximum shear yield strength τ y at this time is 4.64KPa. According to the relationship curve of zero-field viscosity-velocity fitted in Fig. 3, the zero-field viscosity η under the working maximum speed of 25mm/s of the damper is calculated to be 1.45pa.s. Considering that the magnetic saturation current is too small, the adjustment range of the current is small, and the magnetic saturation current is too large, the damper power is large, and it is easy to get hot, so I max is selected as 1.5A in comprehensive consideration. According to mechanical design specifications, material mechanical properties and damper stress, the strength limit of piston rod diameter d is 10.23mm (piston rod opening 4mm), and the strength limit of outer cylinder thickness t is 3.05mm.

依据图1所示的流程框图对磁流变阻尼器进行统一优化设计,当进行磁流变阻尼器设计时,先给定设计目标,然后依据所选材料性能进行几何设计,再在几何设计的基础上进行磁路设计,比较设计参数以得到最终的参数设计值。整个过程基于MATLAB和ANSYS两个软件的仿真结果互换,计算的几何设计和磁路设计的目标值,若不满足设计要求,再返回重新取值、仿真、比较,直到满足设计要求为止。According to the flow chart shown in Figure 1, the unified optimization design of the magnetorheological damper is carried out. When designing the magnetorheological damper, the design goal is first given, and then the geometric design is carried out according to the properties of the selected materials, and then the geometric design is carried out. Based on the magnetic circuit design, compare the design parameters to get the final parameter design value. The whole process is based on the exchange of the simulation results of MATLAB and ANSYS, and the calculated target values of the geometric design and magnetic circuit design, if they do not meet the design requirements, go back to re-take, simulate, and compare until the design requirements are met.

本发明方法中最大阻尼力和可调系数的计算公式如下:The calculation formula of maximum damping force and adjustable coefficient in the inventive method is as follows:

式中, p0=1.2Mpa。In the formula, p 0 =1.2 MPa.

本发明方法中磁路ANSYS有限元仿真的具体分析过程为:(1)选用二维静态分析类型,单元选用二维8节点四边形实体单元Plane53;(2)根据已知材料的导磁特性分别建立活塞、缸筒、间隙磁流变液、线圈、空气和密封环氧树脂部分的有限元模型;(3)在模型外边界线施加磁通量平行的边界条件,划分网格;(4)以电流密度(总电流除以线圈面积)的形式施加激励,对该模型进行静态求解;(5)进入后处理,查看磁场强度数据,进行工作间隙处平均磁感应强度的计算。The specific analysis process of magnetic circuit ANSYS finite element simulation in the method of the present invention is: (1) select the two-dimensional static analysis type for use, and the unit selects the two-dimensional 8-node quadrilateral solid element Plane53 for use; (2) establish respectively according to the magnetic permeability characteristic of known material The finite element model of the piston, cylinder, gap magnetorheological fluid, coil, air and sealing epoxy resin; (3) apply the boundary condition parallel to the magnetic flux on the outer boundary line of the model, and divide the grid; (4) use the current density ( Apply excitation in the form of dividing the total current by the area of the coil) to solve the model statically; (5) enter the post-processing, check the magnetic field intensity data, and calculate the average magnetic induction intensity at the working gap.

可见,磁流变阻尼器的统一优化设计过程实际是不断调整参数直至满足设计要求的过程。经过反复循环上述设计过程,综合实际工程状况,最终确定阻尼器的参数尺寸,详见表1。此时阻尼器计算目标值为:FMRD,max=1557.17N,β0=1.23,本发明方法可操作性强,为磁流变阻尼器的设计提供了理论指导,便于其工程应用和推广。It can be seen that the unified optimization design process of magnetorheological dampers is actually a process of continuously adjusting parameters until the design requirements are met. After repeating the above design process and considering the actual engineering conditions, the parameter size of the damper is finally determined, see Table 1 for details. At this time, the calculated target value of the damper is: F MRD, max = 1557.17N, β 0 = 1.23, The method of the invention has strong operability, provides theoretical guidance for the design of the magneto-rheological damper, and is convenient for its engineering application and popularization.

表1磁流变阻尼器的主要参数尺寸Table 1 Main parameters and dimensions of magnetorheological dampers

显然,上述实施例仅仅是为清楚地说明本发明所作的举例,而并非是对本发明的实施方式的限定。对于所属领域的普通技术人员来说,在上述说明的基础上还可以做出其它不同形式的变化或变动。这里无需也无法对所有的实施方式予以穷举。而这些属于本发明的精神所引伸出的显而易见的变化或变动仍处于本发明的保护范围之中。Apparently, the above-mentioned embodiments are only examples for clearly illustrating the present invention, rather than limiting the implementation of the present invention. For those of ordinary skill in the art, on the basis of the above description, other changes or changes in different forms can also be made. It is not necessary and impossible to exhaustively list all the implementation manners here. And these obvious changes or modifications derived from the spirit of the present invention are still within the protection scope of the present invention.

Claims (7)

1. a kind of Reverse optimization design method of MR damper, it is characterised in that:This method passes through the maximum needed for determination Damping force and adjustability coefficients, geometry designs and magnetic Circuit Design are united and carry out Reverse optimization design, until magnetorheological damping Device meets required maximum damping force and adjustability coefficients under relatively small size;Wherein, geometry designs are emulated using MATLAB Software computational geometry design object value, magnetic Circuit Design utilizes ANSYS finite element stimulation magnetic Circuit Design desired values.
2. the Reverse optimization design method of MR damper according to claim 1, it is characterised in that:Specifically include as Lower step:
Step 1, the design object value of MR damper is selected:Maximum damping force U*With adjustability coefficients β0
Step 2, the maximal rate of damper rod needed for being determined according to actual vibration situationIn conjunction with the magnetorheological of selection Liquid and magnetic circuit material determine the corresponding maximum shear yield strength τ in magnetic flow liquid operating pointyWith null field viscosities il;
Step 3, the maximum damping force U determined according to step 1*, it is living needed for being calculated according to Machine Design specification and characteristic of material mechanics Stopper rod diameter d and outer shell barrel thickness t intensity limit value;
Step 4, the permeance of each material is determined and according to the maximum shear yield strength τ selected in step 2ySearch magnetic circuit Magnetic induction density B is needed at working clearance0
Step 5, the diameter of piston rod d determined according to step 3 intensity limit value carries out geometry designs;
Step 6, institute's need at the magnetic circuit working clearance that the outer shell barrel thickness t determined according to step 3 intensity limit value and step 4 is determined Magnetic induction density B0Carry out magnetic Circuit Design;
Step 7, judge whether the geometric parameter and magnetic circuit parameters of design meet requirement, the repeat step 5 if being unsatisfactory for requiring ~6, until geometric parameter and magnetic circuit parameters reach minimum dimension and meet the design maximum damping force U determined in step 1*With can Adjust factor beta0Requirement.
3. the Reverse optimization design method of MR damper according to claim 2, it is characterised in that:In step 5, institute Stating the design procedure of geometry designs includes:(1) it is preliminary to choose physical dimension parameter piston diameter D, diameter of piston rod d, workplace Gap width h and piston effective length L;(2) calculated and obtained most under the initial parameter currently chosen using MATLAB simulation softwares Big damping force and adjustability coefficients;(3) numerical value and by (2) obtained is compared with design object value, if being unsatisfactory for design requirement, again Physical dimension parameter is chosen, (1)~(3) are repeated, untill numerical value that simulation calculation is obtained meets design requirement;(4) when The numerical value that simulation calculation is obtained is met after design requirement, then judges whether the initial parameter of setting can further reduce, if Smaller value repeat step (1)~(4) can be then chosen again, otherwise choose the parameter set as design result.
4. the Reverse optimization design method of MR damper according to claim 2, it is characterised in that:In step 6, institute Stating the design procedure of magnetic Circuit Design includes:(1) according to geometry designs result, it is preliminary choose determine turn number N, outer shell barrel thickness t, Grooving length a and width b;(2) average magnetic induction intensity at the ANSYS finite element stimulation working clearances is utilized(3) judge Whether grooving length a and width b is less than limit value, carries out next step if meeting, otherwise re-starts geometry designs and carry out Step (1)~(3);(4) average magnetic induction intensity at the working clearance in judgment step (2)Whether selected magnetic is more than or equal to Magnetic induction density B at the working clearance of road0, if it is satisfied, then carrying out next step, otherwise repeat step (1)~(4);(5) judge to set Whether fixed initial parameter can further reduce, if can if choose smaller value repeat step (1)~(5) again, otherwise The parameter set is chosen as design result.
5. the Reverse optimization design method of MR damper according to claim 4, it is characterised in that:Consider that grooving is long A and width b mechanical characteristic requirement is spent, grooving length a limit value takes a quarter of piston head length, grooving width b limit Value takes 1/2nd of piston head diameter and diameter of piston rod difference.
6. the Reverse optimization design method of MR damper according to claim 4, it is characterised in that:The ANSYS The concrete analysis process of finite element simulation is:(1) two-dimensional static analysis type is selected, unit is real from two-dimentional 8 Node Quadrilateral Element Body unit Plane53;(2) piston, cylinder barrel, gap magnetic flow liquid, coil, sky are set up according to the permeance of known materials respectively Gas and the FEM model of sealing epoxy resin part;(3) boundary line applies the parallel boundary condition of magnetic flux outside model, draws Subnetting lattice;(4) apply excitation in the form of current density, static solution is carried out to the model;(5) enter post processing, check magnetic Field strength degrees of data, is operated gap location average magnetic induction intensityCalculating.
7. the Reverse optimization design method of MR damper according to claim 1 or 2, it is characterised in that:It is described most Big damping force and the calculation formula of adjustability coefficients are as follows:
<mrow> <msub> <mi>F</mi> <mrow> <mi>M</mi> <mi>R</mi> <mi>D</mi> <mo>,</mo> <mi>max</mi> </mrow> </msub> <mo>=</mo> <msub> <mi>F</mi> <mi>&amp;tau;</mi> </msub> <mo>+</mo> <msub> <mi>F</mi> <mi>&amp;eta;</mi> </msub> <mo>+</mo> <msub> <mi>F</mi> <msub> <mi>p</mi> <mn>0</mn> </msub> </msub> <mo>;</mo> </mrow>
<mrow> <mi>&amp;beta;</mi> <mo>=</mo> <mfrac> <msub> <mi>F</mi> <mi>&amp;tau;</mi> </msub> <mrow> <msub> <mi>F</mi> <mi>&amp;eta;</mi> </msub> <mo>+</mo> <msub> <mi>F</mi> <msub> <mi>p</mi> <mn>0</mn> </msub> </msub> </mrow> </mfrac> <mo>;</mo> </mrow>
In formula, p0=1.2Mpa.
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