CN108693055B - Method for acquiring material fatigue performance of thin sheet sample - Google Patents

Method for acquiring material fatigue performance of thin sheet sample Download PDF

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CN108693055B
CN108693055B CN201810648886.9A CN201810648886A CN108693055B CN 108693055 B CN108693055 B CN 108693055B CN 201810648886 A CN201810648886 A CN 201810648886A CN 108693055 B CN108693055 B CN 108693055B
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刘勤
蔡力勋
陈辉
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Abstract

本发明公开了一种薄片试样的材料疲劳性能获取方法,包括以下步骤:步骤1:完成薄片试样在应变控制下的多级应变幅的拉压对称循环加载试验,获得循环稳定的载荷‑位移曲线;步骤2:连接载荷‑位移曲线滞回环尖点作为循环载荷‑位移曲线,以循环载荷‑位移关系预测符合Ramberg‑Osgood本构模型的循环应力‑应变关系;步骤3:以循环应力‑应变关系为材料参数,建立疲劳源RVE真实应变幅ε r、应力幅σ r与测控应变幅ε eq 的关系;步骤4:根据ε rσ r 建立疲劳寿命估算模型,获得材料疲劳性能;本发明克服了传统疲劳性能试验检测方法的材料尺寸限制,也不需要依赖经验公式,适用于不同的材料及试样构型。

Figure 201810648886

The invention discloses a method for obtaining material fatigue properties of a thin-film sample, comprising the following steps: Step 1: complete a tension-compression symmetrical cyclic loading test of a multi-level strain amplitude of the thin-film sample under strain control, and obtain a cyclically stable load- Displacement curve; Step 2: Connect the hysteresis loop cusps of the load-displacement curve as the cyclic load-displacement curve, and use the cyclic load-displacement relationship to predict the cyclic stress-strain relationship conforming to the Ramberg-Osgood constitutive model; Step 3: Use the cyclic stress-displacement relationship The strain relationship is a material parameter, and the relationship between the real strain amplitude ε r of the fatigue source RVE, the stress amplitude σ r and the measured and controlled strain amplitude ε eq is established; Step 4: Establish a fatigue life estimation model according to ε r and σ r to obtain the material fatigue performance; The invention overcomes the material size limitation of the traditional fatigue performance test detection method, and does not need to rely on empirical formulas, and is suitable for different materials and sample configurations.

Figure 201810648886

Description

薄片试样的材料疲劳性能获取方法Method for obtaining material fatigue properties of thin specimens

技术领域technical field

本发明涉及疲劳性能测试领域,具体介绍了一种薄片试样的材料疲劳性能获取方法。The invention relates to the field of fatigue performance testing, and specifically introduces a method for obtaining material fatigue performance of thin-film samples.

背景技术Background technique

作为结构稳定性与系统安全评价的基本内容,材料的疲劳力学性能对工程安全分析具有重要意义。表征材料的低周疲劳性能主要包括材料的低循环应力-应变关系与疲劳寿命曲线:前者描述了材料在弹塑性疲劳加载下力学行为的本质物理关系,是循环加载下服役结构的强度分析等具有重要意义;后者描述材料在循环载荷下的服役状态,是对材料或结构进行寿命评估与安全评价的基本曲线。As the basic content of structural stability and system safety evaluation, the fatigue mechanical properties of materials are of great significance to engineering safety analysis. The low-cycle fatigue properties of a material mainly include the low-cycle stress-strain relationship and the fatigue life curve of the material: the former describes the intrinsic physical relationship of the mechanical behavior of the material under elastoplastic fatigue loading, and is the strength analysis of the service structure under cyclic loading. Importance; the latter describes the service state of materials under cyclic loading, and is the basic curve for life assessment and safety assessment of materials or structures.

大量机构或零部件长期经受温度、压力等的循环载荷作用,对关键结构的材料疲劳性能对于系统的安全评价和失效分析十分必要。然而,一方面因小型器件或薄壁管道在生活、生产中的广泛应用,如微机电系统、生物医学工程、新能源系统,由于材料尺寸的限制,很难满足传统测试方法的取样要求;另一方面,为满足现役结构的微损取样剩余寿命检测需求,如飞机发动机叶片与反应堆、锅炉、管道等,采用已有疲劳试验手段很难完成该任务。A large number of mechanisms or components are subjected to cyclic loads such as temperature and pressure for a long time, and the material fatigue performance of key structures is necessary for system safety evaluation and failure analysis. However, on the one hand, due to the wide application of small devices or thin-walled pipes in life and production, such as microelectromechanical systems, biomedical engineering, and new energy systems, due to the limitation of material size, it is difficult to meet the sampling requirements of traditional testing methods; On the one hand, in order to meet the residual life detection requirements of micro-damage sampling of active structures, such as aircraft engine blades and reactors, boilers, pipes, etc., it is difficult to complete this task by using existing fatigue test methods.

薄片试样疲劳性能测试是一种近三十年来用于材料疲劳性能测试的方法,薄片试样的疲劳性能试验研究已有三十余年的历史,自上世纪八十年代开始,Martin(MartinJ.E,Cyclic Stress-Strain and Fatigue Properties of Sheet Steel as Affected byLoad Spectra[J].Testing and Evaluation.1983.66-74.)和Wisner(Wisner SB,Reynolds MB,Adamson RB.Fatigue Behavior of Irradiated and UnirradiatedZircaloy and Zirconium[J].American Society for Testing and Materials,1994.499-520)等设计了漏斗圆弧板状试样开展了对称循环试验,分别利用厚度方向与宽度方向的平均应变进行循环控制试验,为研究薄板的疲劳研究提供试样构型设计及试验技术支持;贾琦、蔡力勋(贾琦.异型试样疲劳与断裂性能测试方法研究与应用[D].西南交通大学,硕士,2011.;贾琦,蔡力勋,包陈.考虑循环塑性修正的薄片材料低周疲劳试验方法[J].工程力学,2014,1:030.)同样采用漏斗板状试样完成了低周疲劳试验,对具有循环Masing效应的材料提出了应变幅稳定阶段应力-应变滞回环上升段作为材料的循环应力-应变关系,完成了对于特殊材料的疲劳寿命的预测;尹涛、蔡力勋等(尹涛,蔡力勋,陈辉,姚迪.基于毫小薄片漏斗试样的材料弹塑性循环本构关系测试方法研究[J].工程力学,2017;尹涛,蔡力勋,陈辉,姚迪.基于毫小薄片试样获取材料应变疲劳性能的测试方法[J].机械工程学报,2017,1:030.)利用毫米厚的漏斗薄片试样的完成材料低周疲劳测试。因外力做功等于变性能该变量,将应变能分为与材料、几何形状及变形量有关的能量分离函数,以变形能为桥梁建立载荷、位移与材料、几何等的关系。能量分离函数如下式:Fatigue performance testing of thin-film specimens is a method used for material fatigue performance testing in the past 30 years. .E,Cyclic Stress-Strain and Fatigue Properties of Sheet Steel as Affected by Load Spectra[J].Testing and Evaluation.1983.66-74.) and Wisner (Wisner SB, Reynolds MB, Adamson RB. Fatigue Behavior of Irradiated and UnirradiatedZircaloy and Zirconium [J]. American Society for Testing and Materials, 1994.499-520) and others designed funnel-arc plate-shaped specimens to carry out symmetrical cyclic tests, using the average strains in the thickness direction and width direction to carry out cyclic control tests, in order to study the thin plate Fatigue research provides sample configuration design and test technical support; Jia Qi, Cai Lixun (Jia Qi. Research and application of fatigue and fracture performance testing methods for special-shaped samples [D]. Southwest Jiaotong University, Master, 2011.; Jia Qi, Cai Lixun , Bao Chen. Low-cycle fatigue test method for thin sheet materials considering cyclic plasticity correction [J]. Engineering Mechanics, 2014, 1:030.) The low-cycle fatigue test was also completed with funnel plate specimens. The material proposes the stress-strain hysteresis loop rising segment in the stable stage of the strain amplitude as the cyclic stress-strain relationship of the material, and completes the prediction of the fatigue life of special materials; Yin Tao, Cai Lixun, etc. (Yin Tao, Cai Lixun, Chen Hui, Yao Di .Research on the testing method of material elastic-plastic cyclic constitutive relation based on micro-slice funnel specimen[J].Engineering Mechanics, 2017; The test method of [J]. Chinese Journal of Mechanical Engineering, 2017, 1:030.) Low-cycle fatigue testing of finished materials using millimeter-thick funnel-sheet specimens. Since the external force work is equal to the variable energy, the strain energy is divided into energy separation functions related to the material, geometry and deformation, and the deformation energy is used as the bridge to establish the relationship between load, displacement and material, geometry, etc. The energy separation function is as follows:

Figure BDA0001699192370000021
Figure BDA0001699192370000021

式中:f1(K)为材料函数,f2(ξ)为几何变形域函数,f3(h)为变形函数,α为塑性等效变形体积系数,β为等效应变系数;根据循环载荷位移关系,反向预测得到符合Ramberg-Osgood本构模型的材料弹性模量E、强度系数K与硬化指数n;In the formula: f 1 (K) is the material function, f 2 (ξ) is the geometric deformation domain function, f 3 (h) is the deformation function, α is the plastic equivalent deformation volume coefficient, β is the equivalent strain coefficient; according to the cycle Load-displacement relationship, reverse prediction to obtain material elastic modulus E, strength coefficient K and hardening exponent n conforming to the Ramberg-Osgood constitutive model;

Figure BDA0001699192370000022
Figure BDA0001699192370000022

其中,η、β、γ为与材料、几何有关的系数。以循环应力应变关系作为材料属性,经有限元计算得到材料在任意应变幅下的根部RVE的应力、应变,完成材料的疲劳寿命预测。Among them, η, β, γ are coefficients related to materials and geometry. Taking the cyclic stress-strain relationship as the material property, the stress and strain of the root RVE of the material under any strain amplitude are obtained by finite element calculation, and the fatigue life prediction of the material is completed.

陈辉、蔡力勋(Hui Chen,Cai Lixun.Theoretical model for predictinguniaxial stress-strain relation by dual conical indentation based onequivalent energy principle[J].Acta Materialia,2016,121:181-189.Hui Chen,CaiLixun.Unified elastoplastic model based on a strain energy equivalenceprinciple[J].Applied Mathematical Modelling,2017,52:664–671;Hui Chen,CaiLixun.Unified ring-compression model for determining tensile properties oftubular materials[J].2017,13:210-220.Peng Y Q,Cai L X,Chen H,et al.A newmethod based on energy principle to predict uniaxial stress-strain relationsof ductile materials by small punch testing[J].International Journal ofMechanical Sciences,2018.)提出了Chen-Cai能量等效方法,经变形域的积分中值等效将变形域总变形能等价为平均变形能与该域体积乘积;由动量定理,外力做功等于内能该变量,建立载荷位移与应变该变量关系:Hui Chen,Cai Lixun(Hui Chen,Cai Lixun.Theoretical model for predicting uniaxial stress-strain relation by dual conical indentation based on equivalent energy principle[J].Acta Materialia,2016,121:181-189.Hui Chen,CaiLixun.Unified elastoplastic model based on a strain energy equivalence principle[J].Applied Mathematical Modelling,2017,52:664–671;Hui Chen,CaiLixun.Unified ring-compression model for determining tensile properties of tubular materials[J].2017,13:210-220. Peng Y Q, Cai L X, Chen H, et al. A new method based on energy principle to predict uniaxial stress-strain relations of ductile materials by small punch testing[J]. International Journal of Mechanical Sciences, 2018.) proposed Chen-Cai energy et al. According to the effective method, the total deformation energy of the deformation domain is equivalent to the product of the average deformation energy and the volume of the domain through the integral median value of the deformation domain; according to the momentum theorem, the work of the external force is equal to the variable of the internal energy, and the relationship between the load displacement and the strain is established. :

Figure BDA0001699192370000023
Figure BDA0001699192370000023

从而建立起载荷-位移关系与应力-应变关系的理论联系。Thereby, the theoretical connection between the load-displacement relationship and the stress-strain relationship is established.

现有技术中,针对薄片漏斗试样完成了低周对称疲劳试验,提供试验条件和试验技术的支持;并给出了薄片漏斗试样特定几何关系(薄片宽度W/漏斗半径R=3)的载荷-位移半解析模型;用于材料循环应力-应变关系的预测,同时完成疲劳寿命预测;但该模型仅针对于有几何相似性的试样构型,对其他试样构型并不具有普适性;Chen-Cai能量等效方法中,给出了能量等效方法的理论指导,并针对不同试样构型的单轴本构关系已有算例,对循环应力-应变关系获取有指导作用。In the prior art, the low-cycle symmetric fatigue test has been completed for the thin-film funnel sample, which provides the support of test conditions and test techniques; and the specific geometric relationship of the thin-film funnel sample (the thin-film width W/funnel radius R=3) is given. Load-displacement semi-analytical model; it is used to predict the cyclic stress-strain relationship of materials and complete the prediction of fatigue life; however, this model is only for the sample configuration with geometric similarity, and it is not common to other sample configurations. In the Chen-Cai energy equivalent method, the theoretical guidance of the energy equivalent method is given, and there are calculation examples for the uniaxial constitutive relationship of different sample configurations, which provides guidance for the acquisition of the cyclic stress-strain relationship effect.

发明内容SUMMARY OF THE INVENTION

本发明提供一种克服传统疲劳性能试验检测方法的材料尺寸限制,不需要依赖经验公式即可获得材料循环应力应变关系并进行材料疲劳寿命预测的薄片试样材料疲劳性能的获取方法。The invention provides a method for obtaining the material fatigue properties of thin slice samples, which overcomes the material size limitation of the traditional fatigue performance test detection method, and can obtain the material cyclic stress-strain relationship and predict the material fatigue life without relying on empirical formulas.

本发明采用的技术方案是:薄片试样的材料疲劳性能获取方法,包括以下步骤:The technical scheme adopted in the present invention is: a method for obtaining material fatigue properties of thin-film samples, comprising the following steps:

步骤1:通过薄片试样在应变控制下的多级应变幅的拉压对称循环加载试验,获得循环稳定的载荷-位移曲线;Step 1: Obtain a cyclically stable load-displacement curve through the symmetric cyclic loading test of the multi-level strain amplitude of the thin sheet under strain control;

步骤2:连接载荷-位移曲线滞回环尖点作为循环载荷-位移曲线,以循环载荷-位移关系预测符合Ramberg-Osgood本构模型的循环应力-应变关系;Step 2: Connect the hysteresis loop cusps of the load-displacement curve as the cyclic load-displacement curve, and use the cyclic load-displacement relationship to predict the cyclic stress-strain relationship conforming to the Ramberg-Osgood constitutive model;

步骤3:以循环应力-应变关系为材料参数,建立疲劳源RVE真实应变幅εr、应力幅σr与测控应变幅εeq的关系;Step 3: Using the cyclic stress-strain relationship as the material parameter, establish the relationship between the fatigue source RVE real strain amplitude ε r , the stress amplitude σ r and the measurement and control strain amplitude ε eq ;

步骤4:根据εr和σr建立疲劳寿命估算模型,获得材料疲劳性能。Step 4: Establish a fatigue life estimation model according to ε r and σ r to obtain material fatigue properties.

进一步的,疲劳源应变幅、应力幅是利用循环应力-应变关系,步骤2的具体过程如下:Further, the fatigue source strain amplitude and stress amplitude are based on the cyclic stress-strain relationship. The specific process of step 2 is as follows:

S1:对循环载荷-位移曲线弹性段进行线性拟合,通过幂律拟合塑性段,分别得到斜率S和加载曲率C及指数m;S1: Linearly fit the elastic segment of the cyclic load-displacement curve, and fit the plastic segment through a power law to obtain the slope S, the loading curvature C and the exponent m, respectively;

Figure BDA0001699192370000031
Figure BDA0001699192370000031

式中:he为弹性位移,h为弹塑性位移,P为外载荷;where: h e is the elastic displacement, h is the elastic-plastic displacement, and P is the external load;

S2:将上式得到的S和C带入下式:S2: Bring the S and C obtained from the above formula into the following formula:

Figure BDA0001699192370000032
Figure BDA0001699192370000032

式中:E为材料的弹性模量,K为应力强度系数,n为应变硬化指数,k0、k1和k2为常数,R为试样中特征长度,A*表示特征面积;where E is the elastic modulus of the material, K is the stress intensity coefficient, n is the strain hardening exponent, k 0 , k 1 and k 2 are constants, R is the characteristic length in the sample, and A* represents the characteristic area;

S3:根据步骤S2中得到的E、K、n代入Ramberg-Osgood模型,得到材料的循环应力-应变关系;S3: Substitute the E, K, and n obtained in step S2 into the Ramberg-Osgood model to obtain the cyclic stress-strain relationship of the material;

Figure BDA0001699192370000041
Figure BDA0001699192370000041

式中:ε为总应变,εe为弹性应变,εp为塑性应变。where ε is the total strain, ε e is the elastic strain, and ε p is the plastic strain.

进一步的,所述k0、k1和k2通过有限元标定获得,且关系如下:Further, the k 0 , k 1 and k 2 are obtained by finite element calibration, and the relationship is as follows:

Figure BDA0001699192370000042
Figure BDA0001699192370000042

式中,a1、a2和a3为k0系数,b1、b2和b3为k1系数,c1、c2和c3为k2系数,λ为几何因子。In the formula, a 1 , a 2 and a 3 are k 0 coefficients, b 1 , b 2 and b 3 are k 1 coefficients, c 1 , c 2 and c 3 are k 2 coefficients, and λ is a geometric factor.

进一步的,所述步骤4中采取Manson-Coffin模型疲劳寿命预测。Further, in the step 4, the Manson-Coffin model fatigue life prediction is adopted.

进一步的,所述试样包括漏斗型试样和圆环形试样。Further, the samples include funnel-shaped samples and annular samples.

进一步的,所述漏斗型试样中,通过有限元建立跨漏斗两侧的测控应变幅εm与漏斗根部真实应变幅εr和平均应力幅σa与真实应力幅σr的转换公式,在低疲劳的应变范围内如下所示:Further, in the funnel-shaped sample, the conversion formulas of the measured and controlled strain amplitude εm across both sides of the funnel, the true strain amplitude εr at the root of the funnel, and the average stress amplitude σa and the true stress amplitude σr are established by finite element. The strain ranges for low fatigue are as follows:

Figure BDA0001699192370000043
Figure BDA0001699192370000043

其中平均应力幅σa=P/A,A为漏斗根部的横截面积,c1~c2、d1~d2是与材料几何尺寸和材料特性有关的系数。Wherein the average stress amplitude σ a =P/A, A is the cross-sectional area of the funnel root, c 1 ~c 2 , d 1 ~d 2 are the coefficients related to the material geometry and material properties.

本发明的有益效果是:The beneficial effects of the present invention are:

(1)本发明方法克服了传统疲劳性能试验检测方法的材料尺寸限制,也不需要依赖经验公式,根据统一与有限元简单标定可准确获得材料循环应力-应变关系,并完成材料疲劳寿命预测,适用于不同的材料及试样构型;(1) The method of the present invention overcomes the material size limitation of the traditional fatigue performance test detection method, and does not need to rely on empirical formulas, and can accurately obtain the cyclic stress-strain relationship of the material according to the unified and simple calibration of the finite element, and complete the material fatigue life prediction, Applicable to different materials and sample configurations;

(2)本发明解决了小型结构件、薄壁管道、焊接材料的疲劳状态和现役结构微损取样剩余寿命检测的关键问题;(2) The present invention solves the key problems of the fatigue state of small structural parts, thin-walled pipes, welding materials and residual life detection of micro-damage sampling of active structures;

(3)本发明对微机电系统、航空、能源系统、生物医学等关键工程领域广泛存在的薄壁结构、微小零部件的材料疲劳力学性能获取具有重要意义。(3) The present invention is of great significance to the acquisition of material fatigue mechanical properties of thin-walled structures and tiny components that widely exist in key engineering fields such as microelectromechanical systems, aviation, energy systems, and biomedicine.

附图说明Description of drawings

图1为本发明实施例采用的试样工作段示意图。FIG. 1 is a schematic diagram of a sample working section adopted in the embodiment of the present invention.

图2为本发明实施例中圆环形试样有限元分析模型。FIG. 2 is the finite element analysis model of the annular sample in the embodiment of the present invention.

图3为本发明中Ramberg-Osgood幂律本构曲线。FIG. 3 is a Ramberg-Osgood power law constitutive curve in the present invention.

图4为本发明实施例中GH4169圆环薄片试样循环载荷-位移曲线。Fig. 4 is the cyclic load-displacement curve of the GH4169 circular ring sheet sample in the embodiment of the present invention.

图5为本发明实施例中GH4169圆环薄片试样循环应力-应变曲线预测结果。FIG. 5 is the predicted result of the cyclic stress-strain curve of the GH4169 annular thin slice sample in the embodiment of the present invention.

具体实施方式Detailed ways

下面结合附图和具体实施例对本发明做进一步说明。The present invention will be further described below with reference to the accompanying drawings and specific embodiments.

一种薄片试样材料疲劳性能的获取方法,包括以下步骤:A method for acquiring fatigue properties of thin-film sample materials, comprising the following steps:

步骤1:对试样进行轴向拉压对称循环试验,获得载荷-位移曲线;Step 1: Perform an axial tension-compression symmetrical cyclic test on the sample to obtain a load-displacement curve;

试样如图1所示采用漏斗形和圆环形两种,其工作段构型图如图1所示;其中圆环形试样有限元分析模型如图2所示;采用微力测试加载装置对漏斗与圆环薄片试样进行拉压对称循环加载,获得每级载荷下的循环次数及每次循环的载荷、位移峰谷值,获取载荷-位移(P-h)曲线;因此薄片试样低周疲劳试验是本发明技术方案中的重要部分;试样在应变控制下完成疲劳试样;为了获取足够的材料低周疲劳信息,材料最小寿命约1000次,最大寿命约10000次,根据材料特性将应变幅分为7级,每级不少于两个试样。As shown in Figure 1, the sample is of funnel shape and annular shape, and its working section configuration diagram is shown in Figure 1; the finite element analysis model of the annular sample is shown in Figure 2; the micro-force test loading device is used Load the funnel and ring sheet specimens symmetrically in tension and compression cycles to obtain the number of cycles under each load and the peak and valley values of load and displacement for each cycle, and obtain the load-displacement (P-h) curve; The fatigue test is an important part of the technical solution of the present invention; the sample is completed under the strain control of the fatigue sample; in order to obtain sufficient low-cycle fatigue information of the material, the minimum life of the material is about 1000 times, and the maximum life is about 10,000 times. The strain amplitude is divided into 7 grades, and each grade is not less than two samples.

步骤2:连接载荷-位移曲线滞回环尖点作为循环载荷-位移曲线,根据Ramberg-Osgood模型得到循环应力-应变关系;Step 2: Connect the hysteresis loop cusps of the load-displacement curve as the cyclic load-displacement curve, and obtain the cyclic stress-strain relationship according to the Ramberg-Osgood model;

S1:对循环载荷-位移曲线弹性段进行线性拟合,通过幂律拟合塑性段,分别得到斜率S和加载曲率C;S1: Linearly fit the elastic segment of the cyclic load-displacement curve, and fit the plastic segment through a power law to obtain the slope S and the loading curvature C respectively;

Figure BDA0001699192370000051
Figure BDA0001699192370000051

式中:he为弹性位移,h为弹塑性位移,P为外载荷;where: h e is the elastic displacement, h is the elastic-plastic displacement, and P is the external load;

S2:将上式得到的S和C带入下式:S2: Bring the S and C obtained from the above formula into the following formula:

Figure BDA0001699192370000052
Figure BDA0001699192370000052

式中:E为材料的弹性模量,K为应力强度系数,n为应变硬化指数,k0、k1和k2为常数,R为试样中特征长度,A*表示特征面积;本发明用到的试样形状结构如图1所示,加载线的A端为固定端,B端为位移加载端;假设特征长度h*=R,R表示圆弧漏斗试样的缺口半径或圆环薄片试样外径;特征体积V*=h*A*,A*表示特征面积,对漏斗试样A*=(2w-πR)t,w为工作段宽度,t为试样厚度;对圆环薄片试样,A*=π(R2-r2),r为试样孔径。In the formula: E is the elastic modulus of the material, K is the stress intensity coefficient, n is the strain hardening index, k 0 , k 1 and k 2 are constants, R is the characteristic length in the sample, and A* represents the characteristic area; The shape and structure of the sample used are shown in Figure 1. The A end of the loading line is the fixed end, and the B end is the displacement loading end; it is assumed that the characteristic length h * = R, and R represents the notch radius or ring of the arc funnel sample The outer diameter of the thin sample; the characteristic volume V * =h * A * , A * represents the characteristic area, for the funnel sample A * =(2w-πR)t, w is the width of the working section, t is the thickness of the sample; Ring sheet sample, A * =π(R 2 -r 2 ), r is the pore size of the sample.

对于不同几何形状的试样用几何因子λ表示,其中对漏斗薄片试样而言,λ=w/R,且λ∈[2.75,4];而圆环薄片试样的λ=r/R,λ∈[0.48,0.72];其中无量纲常数k0、k1和k2可通过有限元分析标定获得,且与几何因子呈二次抛物律关系:Specimens with different geometric shapes are represented by the geometric factor λ, where for the funnel sheet specimen, λ=w/R, and λ∈[2.75,4]; and for the ring sheet specimen, λ=r/R, λ∈[0.48, 0.72]; in which the dimensionless constants k 0 , k 1 and k 2 can be obtained through finite element analysis and calibration, and have a quadratic parabolic relationship with the geometric factor:

Figure BDA0001699192370000061
Figure BDA0001699192370000061

根据测量需求,可分别选取漏斗薄片试样的加载线位移、跨漏斗两侧位移与漏斗根部横向位移,也可采用圆环试样的加载线上位移或圆环横向位移,相关拟合参数如表1所示:According to the measurement requirements, the loading line displacement of the funnel sheet sample, the displacement across the two sides of the funnel and the lateral displacement of the funnel root can be selected respectively, and the loading line displacement of the ring sample or the lateral displacement of the ring can be selected. Table 1 shows:

表1.参数列表Table 1. List of parameters

Figure BDA0001699192370000062
Figure BDA0001699192370000062

对于其他几何构型,只需在有限元重新标定k0、k1和k2,该模型仍然适用。For other geometries, just recalibrate k 0 , k 1 and k 2 in the finite element and the model still works.

S3:根据步骤S2中得到的E、K、n代入Ramberg-Osgood模型,得到材料的循环应力-应变关系;S3: Substitute the E, K, and n obtained in step S2 into the Ramberg-Osgood model to obtain the cyclic stress-strain relationship of the material;

Figure BDA0001699192370000063
Figure BDA0001699192370000063

式中:ε为总应变,εe为弹性应变,εp为塑性应变。where ε is the total strain, ε e is the elastic strain, and ε p is the plastic strain.

本发明选择对屈服区描述较好的Ramberg-Osgood(R-O)应力-应变关系模型;The present invention selects a Ramberg-Osgood (R-O) stress-strain relationship model that describes the yield zone better;

ε=εep ε=ε ep

Figure BDA0001699192370000064
Figure BDA0001699192370000064

Figure BDA0001699192370000065
Figure BDA0001699192370000065

步骤3:根据循环应力-应变关系建立疲劳源RVE真实应变幅εm、应力幅σm与平均应变幅εeq的关系;Step 3: According to the cyclic stress-strain relationship, establish the relationship between the real strain amplitude ε m of the fatigue source RVE, the stress amplitude σ m and the average strain amplitude ε eq ;

步骤4:根据εm和σm建立疲劳寿命估算模型,获得材料疲劳性能。Step 4: Establish a fatigue life estimation model according to ε m and σ m to obtain material fatigue properties.

应变幅-寿命曲线是用于材料或结构疲劳寿命评价的基本曲线,现有标准已经给出了获取方法;其关键是获取疲劳源RVE(Representative Volume Element,材料代表性体积单元)真实应变幅与应力幅;根据材料循环应力-应变关系作为材料属性进行简单有限元弹塑性计算,建立疲劳源RVE真实应变幅εm、应力幅σm与平均应变幅εeq的关系,根据εm和σm建立疲劳寿命Manson-Coffin估算模型,完成寿命预测,获得材料疲劳性能。The strain amplitude-life curve is the basic curve for evaluating the fatigue life of materials or structures, and the existing standards have given the acquisition method; the key is to obtain the actual strain amplitude of the fatigue source RVE (Representative Volume Element, material representative volume element) and Stress amplitude: According to the material cyclic stress-strain relationship as material properties, simple finite element elastoplastic calculation is performed to establish the relationship between the fatigue source RVE real strain amplitude ε m , stress amplitude σ m and average strain amplitude ε eq , according to ε m and σ m Establish the fatigue life Manson-Coffin estimation model, complete the life prediction, and obtain the material fatigue properties.

具体实施例specific embodiment

本发明以漏斗薄片试样和圆环薄片的疲劳性能测试为例。试样分为夹持段与工作段,两种试样的工作段如图1所示。建立有限元仿真模型,工作段网格模型如图2所示,一端采用固定铰接,另一端单向加载。采用Ramberg-Osgood本构模型作为材料属性进行计算,该模型曲线如图3,包含弹性模量、强化系数及硬化指数,改变不同材料参数及几何构型参数进行多种工况的有限元模拟,得到对应载荷-位移曲线,并标定弹、塑性系数。The present invention takes the fatigue performance test of the funnel sheet sample and the ring sheet as an example. The sample is divided into a clamping section and a working section, and the working sections of the two kinds of samples are shown in Figure 1. A finite element simulation model is established. The mesh model of the working section is shown in Figure 2. One end is fixedly hinged, and the other end is loaded in one direction. The Ramberg-Osgood constitutive model is used to calculate the material properties. The model curve is shown in Figure 3, which includes elastic modulus, strengthening coefficient and hardening index. Different material parameters and geometric configuration parameters are changed to carry out finite element simulation of various working conditions. The corresponding load-displacement curve is obtained, and the elastic and plastic coefficients are calibrated.

利用GH4169材料的漏斗薄片试样完成应变控制下的拉压对称疲劳试验,厚度t=0.5mm,圆弧半径R=1.2mm,工作段宽度w=3.6mm;引伸计刀口在跨漏斗两侧,采集漏斗两侧位移,用h表示,图4为循环稳定的载荷-位移滞回曲线,连接滞回环尖点为循环载荷位移特征曲线。The tension-compression symmetric fatigue test under strain control was completed by using the funnel sheet sample of GH4169 material, the thickness t=0.5mm, the arc radius R=1.2mm, and the working section width w=3.6mm; The displacement on both sides of the collection funnel is represented by h. Figure 4 shows the cyclically stable load-displacement hysteresis curve, and the cusp of the connecting hysteresis loop is the cyclic load-displacement characteristic curve.

将曲线的线性段用直线拟合,纯塑性部分用幂律拟合,得到Ramberg-Osgood本构模型参数弹性模量E、强化系数K、硬化指数n,将得到的E、K、n代入模型得到材料的循环应力-应变关系;根据不同薄片试样预测的循环应力-应变曲线与同材料的等值圆棒疲劳试验预测结果如图5所示,不同薄片试样的循环应力-应变曲线基本重合于等值圆棒的结果。在实际使用时,依据材料尺寸及试验条件,试样大小与几何比例均可调整,工作段不同几何构型的参数也可以用有限元简单计算得到。利用该循环应力-应变关系得到材料真实应力、应变,根据应力、应变的疲劳寿命预测方法比较常用,不再赘述。The linear segment of the curve is fitted with a straight line, and the pure plastic part is fitted with a power law to obtain the parameters of the Ramberg-Osgood constitutive model: elastic modulus E, strengthening coefficient K, and hardening exponent n, and substitute the obtained E, K, and n into the model The cyclic stress-strain relationship of the material is obtained; the cyclic stress-strain curves predicted according to different thin samples and the predicted results of the equivalent round bar fatigue test of the same material are shown in Figure 5. The cyclic stress-strain curves of different thin samples are basically Coinciding with the results of the equivalent round bars. In actual use, the sample size and geometric ratio can be adjusted according to the material size and test conditions, and the parameters of different geometric configurations of the working section can also be simply calculated by finite element. Using the cyclic stress-strain relationship to obtain the true stress and strain of the material, the fatigue life prediction method based on the stress and strain is more commonly used, and will not be repeated here.

本发明采用微力测试加载装置对漏斗与圆环薄片试样进行拉压对称循环加载,获得每级荷载下的循环次数及每次循环的载荷、位移峰谷值,通过每级循环稳定(Nf/2)的载荷-位移滞回曲线预测材料的循环应力-应变关系,并以此为基础建立εeqm与εeqm关系,完成Manson-Coffin疲劳寿命预测;本发明克服了传统疲劳性能试验检测方法的材料尺寸限制,不需依赖经验公式,可较为准确的获得材料循环应力-应变关系,完成对材料的疲劳寿命预测;解决了小型结构件、焊接材料的疲劳性能获取和现役结构微损取样剩余寿命检测的关键性技术问题;对微机电系统、航空、能源系统、生物医学等关键工程广泛存在的薄壁结构、微小零部件的材料疲劳力学性能和现役材料疲劳寿命的预测获取具有重要意义。In the present invention, the micro-force test loading device is used to load the funnel and the circular ring sheet sample in a tension-compression symmetrical cycle to obtain the number of cycles under each level of load and the load and displacement peak and valley values of each cycle . /2) The cyclic stress-strain relationship of the material is predicted by the load-displacement hysteresis curve, and the relationship between ε eqm and ε eqm is established on this basis to complete the Manson-Coffin fatigue life prediction; the invention overcomes the The material size limitation of the traditional fatigue performance testing method does not need to rely on empirical formulas, and can obtain the cyclic stress-strain relationship of the material more accurately, and complete the fatigue life prediction of the material; The key technical issues in the residual life detection of micro-damage sampling of active structures; Predictive acquisition is important.

Claims (5)

1. A method for acquiring material fatigue performance of a sheet sample is characterized by comprising the following steps:
step 1: obtaining a load-displacement curve with stable circulation through a tension-compression symmetrical cyclic loading test of a sheet sample under the strain control in a multistage strain amplitude;
step 2: connecting the hysteresis loop sharp points of the load-displacement curve as a cyclic load-displacement curve, and predicting the cyclic stress-strain relation which accords with the Ramberg-Osgood constitutive model according to the cyclic load-displacement relation;
and step 3: the circulation stress-strain relation is taken as a material parameter to establish the RVE real strain amplitude of the fatigue sourcerStress amplitude σrAnd measure and control strain amplitudeeqThe relationship of (1);
and 4, step 4: according torAnd σrEstablishing a fatigue life estimation model to obtain the fatigue performance of the material;
the specific process of the step 2 is as follows:
s1: performing linear fitting on the cyclic load-displacement curve elastic segment, and respectively obtaining a slope S, a loading curvature C and an index m through power law fitting on the plastic segment;
Figure FDA0002463334750000011
in the formula: h iseElastic displacement, h elastic-plastic displacement and P external load;
s2: substituting S and C from the above formula into the following formula:
Figure FDA0002463334750000012
in the formula: e is the elastic modulus of the material, K is the stress intensity coefficient, n is the strain hardening index, K0、k1And k2Is constant, R is the characteristic length of the sample, and A represents the characteristic area;
s3: substituting E, K, n obtained in the step S2 into a Ramberg-Osgood model to obtain a cyclic stress-strain relation of the material;
Figure FDA0002463334750000013
in the formula: in order to be the total strain,ein order to be elastically strained,pis a plastic strain.
2. The method for obtaining the material fatigue property of the thin slice sample according to claim 1, wherein the k is0、k1And k2Obtained by finite element calibration and the relationship is as follows:
Figure FDA0002463334750000014
in the formula, a1、a2And a3Is k0Coefficient, b1、b2And b3Is k1Coefficient, c1、c2And c3Is k2The coefficient, λ, is the geometric factor.
3. The method for acquiring the material fatigue property of the flake sample according to claim 1, wherein a Manson-coffee model fatigue life prediction is adopted in the step 4.
4. The method for acquiring the material fatigue property of the thin slice sample as claimed in claim 1, wherein the sample comprises a funnel-shaped sample and a circular ring-shaped sample.
5. The method for obtaining material fatigue performance of thin slice sample according to claim 4, wherein in the funnel-shaped sample, the measurement and control strain amplitude across two sides of the funnel is established by finite elementsmAmplitude of true strain of funnel rootrAnd the mean stress amplitude σaWith the true stress amplitude sigmarThe transformation formula of (c) in the low fatigue strain range is as follows:
Figure FDA0002463334750000021
wherein the mean stress amplitude σaP/A, A is the cross-sectional area of the root of the funnel, c1~c2、d1~d2Is a coefficient related to the material geometry and material properties.
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