WO2021098169A1 - Method for predicting fatigue life of geometrically discontinuous structure - Google Patents

Method for predicting fatigue life of geometrically discontinuous structure Download PDF

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WO2021098169A1
WO2021098169A1 PCT/CN2020/091262 CN2020091262W WO2021098169A1 WO 2021098169 A1 WO2021098169 A1 WO 2021098169A1 CN 2020091262 W CN2020091262 W CN 2020091262W WO 2021098169 A1 WO2021098169 A1 WO 2021098169A1
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fatigue
slip
discontinuous structure
plastic
equation
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PCT/CN2020/091262
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French (fr)
Chinese (zh)
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张显程
苑光健
王润梓
涂善东
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华东理工大学
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    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F30/00Computer-aided design [CAD]
    • G06F30/20Design optimisation, verification or simulation
    • G06F30/23Design optimisation, verification or simulation using finite element methods [FEM] or finite difference methods [FDM]
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F2119/00Details relating to the type or aim of the analysis or the optimisation
    • G06F2119/14Force analysis or force optimisation, e.g. static or dynamic forces

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  • the invention relates to the field of life prediction for structures containing notches, and in particular to a fatigue life prediction method based on ABAQUS.
  • the ABAQUS finite element commercial software can not only analyze complex fixed mechanics and structural mechanics systems, but also supplement the imperfect functions of the ABAQUS pre-processing module through a powerful secondary development interface.
  • the user-defined subroutine based on FORTRAN language expands the application of ABAQUS in constitutive equations, and realizes the functions of damage assessment and life prediction.
  • the user-defined subroutines adapted from the Fortran language can better compile the required constitutive model according to your own materials or needs.
  • fatigue analysis and life prediction of complex structures can mainly describe the continuous damage mechanics theory including crack initiation and propagation stages, which introduces a unified fatigue constitutive through damage variables to describe the process of damage accumulation to fracture under cyclic loading. .
  • This type of method focuses on describing the fatigue behavior in the crack propagation stage. Its complex programming, poor convergence, and high computational cost determine that this type of method does not have a strong universality. In addition, this method is aimed at macro-level components and has a strong impact on micro-level components. The layer stress-strain response and mechanism analysis are not accurate. Due to the initiation of cracks, it is usually produced on a microscopic level. Therefore, how to more effectively evaluate the crack initiation life and analyze the causes of crack initiation is very important.
  • the present invention provides a method for predicting the fatigue life of geometrically discontinuous structures, which can better realize the fatigue analysis of geometrically discontinuous structures, and has the advantages of intuitiveness, strong applicability, and high accuracy.
  • the present invention provides a method for predicting the fatigue life of a geometrically discontinuous structure, which includes the following steps:
  • step S4 Establish a second ABAQUS finite element model of the geometric discontinuous structure, and combine the user subroutine UMAT of step S1 with the material parameters and fatigue plastic slip critical value of step S3, and use ABAQUS software to simulate the cycle Load uniaxial fatigue test to obtain the stress-strain relationship and single-cycle fatigue plastic slip value for each cycle;
  • step S5 Combining the critical fatigue plastic slip value of step S3 and the single-cycle fatigue plastic slip value of step S4, calculate the crack initiation life of the notched sample.
  • the crystal plasticity constitutive equation includes a master control equation, a slip flow criterion equation, and a back stress evolution equation.
  • step S1 includes:
  • F is the total deformation gradient
  • F e is the elastic deformation gradient
  • F p is the inelastic deformation gradient
  • L is the deformation rate gradient
  • Le is the elastic deformation rate gradient
  • L p is the inelastic deformation rate gradient
  • Is the plastic slip rate of the ⁇ -th slip system
  • s ⁇ is the slip direction vector of the ⁇ -th slip system
  • m ⁇ is the normal direction vector of the ⁇ -th slip system
  • F 0 is the thermal activation free energy
  • k is Boltzmann’s constant
  • is the absolute temperature
  • ⁇ ⁇ is the decomposed shear stress of the ⁇ -th slip system
  • is the stress value
  • B ⁇ is the first The back stress of the ⁇ slip system
  • ⁇ and ⁇ 0 are the shear modulus at ⁇ and 0K, respectively
  • ⁇ 0 , p, q are the material constants
  • S ⁇ is the slip resistance of the ⁇ -th slip system
  • h s and d D is the static hardening and dynamic recovery modulus respectively
  • h B is the back-stress hardening constant
  • r D is the dynamic recovery coefficient related to slip resistance
  • f c is the coupling parameter related to internal variables
  • ⁇ ′ 0 is the local slip shear modulus at 0K
  • is the material constant.
  • the shape of the sample used in the uniaxial tensile test and the uniaxial fatigue test is the same as the shape of the first ABAQUS finite element model in the step S1.
  • the fatigue damage calculation model is established according to the first ABAQUS finite element model and the crystal plasticity constitutive equation in the step S1.
  • the fatigue plastic slip critical value P crit is:
  • L p is the inelastic deformation rate gradient
  • P crit is the critical value of fatigue plastic slip
  • step S4 when simulating the uniaxial fatigue test of the cyclic load, the calculation formula adopts the crystal plastic constitutive equation defined by the user subroutine UMAT in the step S1, and the applied cyclic load The load is the same as that of the uniaxial fatigue test in step S2.
  • step S4 further includes: after establishing the second ABAQUS finite element model of the geometric discontinuous structure, applying reasonable boundary conditions and external loads to divide the model mesh.
  • the crack initiation life is:
  • N i is the initiation of fatigue life
  • P crit plastic slip fatigue threshold P cyc single cycle fatigue plastic slip value.
  • the present invention uses the fatigue plastic slip critical value P crit as the fatigue indicator, and can use micro-scale parameters as damage parameters to evaluate life.
  • the advantage of this method lies in the prediction on the micro-scale. Not only can the life be predicted, but also the accumulation map of plastic slip damage in each cycle can be obtained, thereby predicting the location of crack initiation.
  • the crystal plasticity constitutive in the user subroutine UMAT used in the fatigue life prediction method of the geometric discontinuous structure of the present invention is based on the classic crystal plasticity theory, and the stress and strain behavior of the geometric discontinuous structure under fatigue load can be obtained, and it adopts
  • the slip flow criterion equation is a temperature-dependent power exponential slip flow criterion, which can simulate not only normal temperature but also high temperature, and can be used to describe the mechanical behavior of different temperature states, thereby making the geometric discontinuity of the present invention
  • the fatigue life prediction method of structure can predict the structure life under high temperature.
  • the invention adopts the ABAQUS finite element model, which has strong intuitiveness, and can intuitively obtain the crack initiation position of the geometric discontinuous structure and predict the crack initiation life of the position.
  • Fig. 1 is a flowchart of a method for predicting fatigue life of a geometrically discontinuous structure according to an embodiment of the present invention
  • FIG. 2 is a schematic diagram of a first ABAQUS finite element model of a method for predicting fatigue life of a geometrically discontinuous structure according to an embodiment of the present invention
  • Fig. 3 is a graph of the uniaxial tensile test and simulation curve fitting results of the method for predicting the fatigue life of a geometric discontinuous structure according to an embodiment of the present invention
  • FIG. 4 is a diagram of the hysteresis loop data of the uniaxial fatigue test and the fitting result diagram of the fitting curve of the fatigue life prediction method of the geometric discontinuous structure according to an embodiment of the present invention
  • Figures 5(a)-5(h) are the finite element model diagrams of different notched specimens used in the fatigue life prediction method of the geometric discontinuous structure of the present invention, wherein Figures 5(a)-5(h) show Different notch sizes;
  • Fig. 6 is a diagram showing the linear growth trajectory of plastic strain accumulated in different cycles of different notched specimens in the fatigue life prediction method of the geometric discontinuous structure of the present invention
  • Figure 7 is a comparison diagram of life prediction for different notched specimens
  • FIG. 8 is a comparison diagram of the life prediction results of different notched specimens and the experimental verification results of the fatigue life prediction method of the geometric discontinuous structure of the present invention.
  • FIG. 9 is a diagram of the relationship between different notch lengths and predicted life predicted by the fatigue life prediction method of the geometric discontinuous structure of the present invention.
  • Fig. 10 is a diagram of the relationship between the different notch areas predicted by the fatigue life prediction method of the geometric discontinuous structure of the present invention and the predicted life.
  • FIG. 1 for a method for predicting fatigue life of a geometrically discontinuous structure disclosed in the present invention, which includes the following steps:
  • the first ABAQUS finite element model refers to a model modeled by the finite element software ABAQUS, the shape of which is shown in FIG. 2, and is used to describe the microstructure information of the material with the geometric discontinuous structure.
  • the crystal plastic constitutive equations include master control equations, slip flow criterion equations, and back stress evolution equations (ie formulas 1 to 11 described below), which are used to describe the stress and strain of the material with the geometric discontinuous structure Relationship and used to embed the first ABAQUS finite element model for finite element calculations.
  • the stress-strain relationship includes an elastic part and a plastic part, and the plastic part is calculated using the crystal plastic constitutive equation.
  • step S1 further includes the steps:
  • F is the total deformation gradient
  • F e is the elastic deformation gradient
  • F p is the inelastic deformation gradient
  • L is the deformation rate gradient
  • Le is the elastic deformation rate gradient
  • L p is the inelastic deformation rate gradient
  • Is the plastic slip rate of the ⁇ -th slip system
  • s ⁇ is the slip direction vector of the ⁇ -th slip system
  • m ⁇ is the normal direction vector of the ⁇ -th slip system
  • the slip flow criterion equation includes:
  • Is the plastic slip rate of the ⁇ -th slip system Is the reference plastic slip rate
  • F 0 is the thermal activation free energy
  • the unit is kJ ⁇ mol -1
  • k is Boltzmann's constant
  • ⁇ (T) is the absolute temperature
  • ⁇ ⁇ is the decomposition shear of the ⁇ -th slip system Stress
  • the unit is MPa
  • the evolution equation is shown in formula (5)
  • is the stress value
  • the unit is MPa
  • B ⁇ is the back stress of the ⁇ -th slip system
  • the unit is MPa
  • ⁇ and ⁇ 0 are respectively ⁇ and 0K
  • the unit of shear modulus at time is GPa
  • ⁇ 0 , p, q are material constants
  • the unit of ⁇ 0 is MPa.
  • S ⁇ is the slip resistance of the ⁇ -th slip system, in MPa. Its evolution equation is shown in formula (6), h s and d D are static hardening and dynamic recovery modulus, respectively, in units of MPa, Is the initial slip resistance of the ⁇ -th slip system, in MPa.
  • the slip flow criterion equation in the crystal plastic constitutive equation used in the fatigue life prediction method of the geometric discontinuous structure of the present invention is a power exponential slip flow criterion, compared with the traditional power function type, heat is embedded Temperature-related parameters such as activation energy can simulate the mechanical behavior of materials at different temperatures.
  • h B is the back stress hardening constant
  • the unit is MPa
  • r D is the dynamic recovery coefficient related to slip resistance
  • the evolution equation is shown in formula (8)
  • f c is the coupling parameter related to internal variables
  • ⁇ ′ 0 is The local slip shear modulus at 0K
  • the unit is GPa
  • is the material constant.
  • the fatigue life prediction method of the geometric discontinuous structure of the present invention adopts the back stress inelastic follow-up strengthening equation, thereby taking into account the temperature effect.
  • S2 Perform a uniaxial tensile test and a uniaxial fatigue test with different strain amplitudes on the material with the geometric discontinuous structure at the same temperature to obtain a tensile curve and a hysteresis loop.
  • the temperatures used are all room temperature, but the method of the present invention can also be applied to various service temperatures of materials.
  • the shape of the sample used in the uniaxial tensile test and the uniaxial fatigue test is the same as the shape of the first ABAQUS finite element model in step S1.
  • the fatigue damage calculation model is established according to the first ABAQUS finite element model and the crystal plasticity constitutive equation in the step S1.
  • L p is the inelastic deformation rate gradient
  • P crit is the critical value of fatigue plastic slip
  • the first ABAQUS finite element model of step S1 is geometrically continuous, that is, it does not contain gaps, it is used for parameter correction. Because the first ABAQUS finite element model can be fitted with the stretch curve and hysteresis loop in step S2, we use the first ABAQUS finite element model without gaps to fit the experiment to determine the parameters.
  • step S4 Establish a second ABAQUS finite element model of the geometric discontinuous structure (that is, including gaps), apply reasonable boundary conditions and external loads, divide the model mesh, and combine the user subroutine UMAT of step S1 with all
  • the material parameters and fatigue plastic slip critical value P crit of step S3 are described.
  • the ABAQUS software is used to simulate the uniaxial fatigue test of cyclic loading, and the stress-strain relationship and single-cycle fatigue of each cycle (each integration point) are obtained.
  • the calculation of plastic slip value and single cycle fatigue plastic slip value also use formulas (9) and (10).
  • the model shape and gap of the geometric discontinuous structure can be changed according to actual engineering conditions. Since it is the life prediction object of the present invention, a second finite element model with gaps is established to predict the life.
  • the total number of cycle cycles may be the total cycle cycles up to the time of fatigue fracture.
  • the calculation formula adopts the crystal plasticity constitutive equation defined by the user subroutine UMAT in step S1, and the applied cyclic load is the same as that of the uniaxial fatigue test in step S2.
  • the load is the same, and the evolution of each cycle is calculated from this.
  • the single-cycle fatigue plastic slip value and the evolution process of plastic slip per cycle as shown in Fig. 6 can be obtained.
  • step S5 Combining the critical fatigue plastic slip value of step S3 and the single-cycle fatigue plastic slip value of step S4, calculate the crack initiation life of the notched sample.
  • the crack initiation life is:
  • N i is the crack initiation life
  • P crit plastic slip fatigue threshold P cyc single cycle fatigue plastic slip value
  • the fatigue life prediction method of geometric discontinuous structure provided by the present invention is used to verify the effectiveness of the present invention for different notched specimens, and the initiation life information of the experiment is used.
  • the material of the notched sample is nickel-based GH4169 superalloy, and the fatigue test is carried out in an air environment at room temperature. The external load applied at both ends of the specimen is the overall stress control. Due to the geometric discontinuity of the unilateral notch specimen, the weakest part of the notch is in a multiaxial stress-strain state.
  • the fatigue life prediction method of the geometric discontinuous structure of the present invention requires uniaxial tensile test under normal temperature air environment and uniaxial fatigue test with different strain amplitudes on samples without notches of the same material.
  • the obtained test The result is used to determine the material parameters required by the crystal plastic constitutive equations of formulas (1) to (8) and (11) in step S2 of the fatigue life prediction method of the geometric discontinuous structure of the present invention.
  • the results are shown in Figure 3 and Figure 4.
  • the critical value P crit of fatigue plastic slip can be determined according to the fitting result, and then the life prediction of materials with different notches can be carried out.
  • Figure 5 (a)- Figure 5 (h) show the ABAQUS model diagrams of different notched samples.
  • the size of the model is the same, and different gap sizes are changed, where a represents the length of the gap and b represents the width of the gap.
  • Figure 6 shows the fatigue cumulative plastic strain trajectory diagram for each cycle of different notched specimens. It can be seen that when the size of the gap is larger, the cumulative plastic slip is also larger. In addition, plastic accumulation is linear, so the above formula (11) can be used to calculate the fatigue initiation life of different specimens.
  • Figure 7 shows the life prediction diagrams of different notched specimens.
  • the fatigue life prediction method of the geometric discontinuous structure of the present invention uses cumulative plastic slip to predict the result of the initiation life, which is relatively close to the experimental result and within the range of 2 times the error band. Therefore, this numerical simulation is proved
  • the method has high reliability.
  • the location of crack initiation can also be predicted. Crack initiation is mainly concentrated in two areas, one is the stress concentration area at the root of the notch. This is because the root of the notch is a potential dangerous point in the fatigue process, and the stress concentration effect is more obvious; the other is at a location far away from the root, where the cracks are located in this area.
  • the initiation is mainly caused by the large plastic deformation of local grains.
  • Figure 8 shows the comparison diagram of the life prediction of different models and the experimental results. It can be seen from the figure that the life comparison of all the prediction results obtained by the present invention and the experimental results are within the range of 2 times the error band, which proves This numerical simulation method has high reliability and stability.
  • the analysis of different notch length and notch area reveals that the life span has a great relationship with notch length and notch area.
  • Figure 9 shows the life comparison diagram of different notch lengths. It can be seen from the figure that as the length of the notch increases, the fatigue life gradually decreases. In addition, after the length reaches a certain value, the life will reach a plateau. The length of the gap in the later period will have a smaller effect.
  • Figure 10 shows the life comparison chart of different notch areas. It can be seen from the figure that as the notch area increases, the fatigue life gradually decreases. After the notch area increases, the plateau phenomenon will also appear. Moreover, there is a certain evolutionary relationship between notch area and fatigue life:
  • A is the area of the notch
  • N i is the fatigue life

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Abstract

A method for predicting the fatigue life of a geometrically discontinuous structure, comprising the steps of: establishing a geometrically continuous first finite element model, defining a crystal plasticity constitutive equation, thereby obtaining a stress-strain relationship of a material under a given cyclic loading condition (S1); carrying out a uniaxial tensile test and a uniaxial fatigue test to obtain a tensile curve and a hysteresis loop (S2); obtaining the tensile curve and hysteresis loop by means of test parameter fitting, and acquiring material parameters and a critical value of fatigue plastic slip required by the crystal plasticity constitutive equation (S3); establishing a second finite element model of the geometrically discontinuous structure, and acquiring a stress-strain relationship of each cycle and a single-cycle fatigue plastic slip value (S4); and calculating the crack initiation life of a notched specimen (S5). The method for predicting the fatigue life of the geometrically discontinuous structure may better achieve the fatigue analysis of the geometrically discontinuous structure at different temperatures, and may also accurately predict the location of crack initiation. The method has the advantages of intuitiveness, strong applicability and high accuracy.

Description

一种几何不连续结构的疲劳寿命预测方法A fatigue life prediction method for geometrically discontinuous structures 技术领域Technical field
本发明涉及含缺口结构的寿命预测领域,尤其涉及一种基于ABAQUS的疲劳寿命预测方法。The invention relates to the field of life prediction for structures containing notches, and in particular to a fatigue life prediction method based on ABAQUS.
背景技术Background technique
在航空发动机制造过程中,由于加工条件、制造工艺和安装条件等客观原因的存在,涡轮盘等重要零件在安装过程中不可避免地存在一些表面微缺陷。此外,在飞机运行过程中,空气中悬浮固体的冲击也会对发动机叶片和涡轮盘等重要部件造成严重损坏。正是由于这些微缺陷和小缺口的存在,加速了航空发动机涡轮盘、叶片等重要部件的疲劳裂纹萌生,降低了发动机部件的疲劳寿命。因此,为了保证经济性和安全性,在发动机零部件存在缺陷的前提下,准确评估发动机构件的正常使用寿命是非常重要的。In the process of aeroengine manufacturing, due to the existence of objective reasons such as processing conditions, manufacturing processes and installation conditions, some important parts such as turbine disks inevitably have some surface micro-defects during the installation process. In addition, during the operation of the aircraft, the impact of suspended solids in the air can also cause serious damage to important components such as engine blades and turbine disks. It is precisely because of the existence of these micro-defects and small gaps that the initiation of fatigue cracks in important parts such as aero-engine turbine discs and blades has been accelerated, and the fatigue life of engine parts has been reduced. Therefore, in order to ensure economy and safety, it is very important to accurately assess the normal service life of engine components under the premise that engine components have defects.
近些年,有限元软件的发展可以很好地满足人们对于复杂应力应变行为的理解以及提供了该状态下精确寿命预测的可行性。ABAQUS有限元商业软件不仅可以分析复杂的固定力学和结构力学系统,还可以通过强大的二次开发接口补充ABAQUS前后处理模块中不完善的功能。其中,基于FORTRAN语言的用户自定义的子程序扩展了ABAQUS在本构方程的应用,并实现了损伤评估、寿命预测等方面的功能。与现有的ABAQUS软件自带的处理模块相比,基于Fortran语言改编的用户自定义子程序,可以更好的根据自己的材料或者需求,来编译所需的本构模型。In recent years, the development of finite element software can satisfy people's understanding of complex stress-strain behavior and provide the feasibility of accurate life prediction in this state. The ABAQUS finite element commercial software can not only analyze complex fixed mechanics and structural mechanics systems, but also supplement the imperfect functions of the ABAQUS pre-processing module through a powerful secondary development interface. Among them, the user-defined subroutine based on FORTRAN language expands the application of ABAQUS in constitutive equations, and realizes the functions of damage assessment and life prediction. Compared with the existing processing modules of the ABAQUS software, the user-defined subroutines adapted from the Fortran language can better compile the required constitutive model according to your own materials or needs.
现今针对复杂结构的疲劳分析及寿命预测的主要能够描述包含裂纹萌生和扩展阶段的连续损伤力学理论,其通过损伤变量引入统一的疲劳本构的方式描述材料在循环载荷下损伤累积直至断裂的过程。这类方法侧重于描述裂纹扩展阶段的疲劳行为,其编程复杂、收敛性差、计算成本高等特点决定了这类方法不具有很强的普适性,此外,这种方法针对宏观层面构件,对微观层面的应力应变响应以及机理分析并不准确。由于裂纹的萌生,通常是从微观层次上产生的。因此,如何更有效的评估裂纹萌生寿命,并分析裂纹萌生的原因,是非常重要的。Nowadays, fatigue analysis and life prediction of complex structures can mainly describe the continuous damage mechanics theory including crack initiation and propagation stages, which introduces a unified fatigue constitutive through damage variables to describe the process of damage accumulation to fracture under cyclic loading. . This type of method focuses on describing the fatigue behavior in the crack propagation stage. Its complex programming, poor convergence, and high computational cost determine that this type of method does not have a strong universality. In addition, this method is aimed at macro-level components and has a strong impact on micro-level components. The layer stress-strain response and mechanism analysis are not accurate. Due to the initiation of cracks, it is usually produced on a microscopic level. Therefore, how to more effectively evaluate the crack initiation life and analyze the causes of crack initiation is very important.
发明内容Summary of the invention
针对上述现有技术中的不足,本发明提供一种几何不连续结构的疲劳寿命预测方法,能够更好地实现几何不连续结构的疲劳分析,具有直观、适用性强、精确度高的优点。In view of the above-mentioned shortcomings in the prior art, the present invention provides a method for predicting the fatigue life of geometrically discontinuous structures, which can better realize the fatigue analysis of geometrically discontinuous structures, and has the advantages of intuitiveness, strong applicability, and high accuracy.
为了实现上述目的,本发明提供一种几何不连续结构的疲劳寿命预测方法,其包括以下步骤:In order to achieve the above objective, the present invention provides a method for predicting the fatigue life of a geometrically discontinuous structure, which includes the following steps:
S1:建立一个几何连续且包含所述几何不连续结构的材料的多个晶粒的第一ABAQUS有限元模型,并通过用户子程序UMAT定义所述材料在循环载荷的单轴疲劳试验的过程中的晶体塑性本构方程,以此得到所述材料在给定的循环载荷条件下的应力应变关系;S1: Establish a geometrically continuous first ABAQUS finite element model containing multiple crystal grains of the material with the geometric discontinuous structure, and define the material during the cyclic load uniaxial fatigue test through the user subroutine UMAT The crystal plasticity constitutive equation of, to obtain the stress-strain relationship of the material under given cyclic loading conditions;
S2:对所述几何不连续结构的材料在同一温度下进行单轴拉伸试验以及不同应变幅的单轴疲劳试验,得到拉伸曲线和迟滞回线;S2: Perform uniaxial tensile test and uniaxial fatigue test with different strain amplitudes on the material with the geometric discontinuous structure at the same temperature to obtain the tensile curve and hysteresis loop;
S3:建立疲劳损伤计算模型,通过试参法拟合获得所述第一ABAQUS有限元模型的拉伸曲线和迟滞回线,进而获取所述晶体塑性本构方程所需的材料参数和疲劳塑性滑移临界值;S3: Establish a fatigue damage calculation model, and obtain the tensile curve and hysteresis loop of the first ABAQUS finite element model through trial-parameter fitting, and then obtain the material parameters and fatigue plastic slip required by the crystal plastic constitutive equation Shift critical value;
S4:建立所述几何不连续结构的第二ABAQUS有限元模型,并结合所述步骤S1的用户子程序UMAT和所述步骤S3的材料参数和疲劳塑性滑移临界值,采用ABAQUS软件来模拟循环载荷的单轴疲劳试验,得到每个循环周次的应力应变关系和单周疲劳塑性滑移值;S4: Establish a second ABAQUS finite element model of the geometric discontinuous structure, and combine the user subroutine UMAT of step S1 with the material parameters and fatigue plastic slip critical value of step S3, and use ABAQUS software to simulate the cycle Load uniaxial fatigue test to obtain the stress-strain relationship and single-cycle fatigue plastic slip value for each cycle;
S5:结合所述步骤S3的疲劳塑性滑移临界值和所述步骤S4的单周疲劳塑性滑移值,计算得到缺口试样的裂纹萌生寿命。S5: Combining the critical fatigue plastic slip value of step S3 and the single-cycle fatigue plastic slip value of step S4, calculate the crack initiation life of the notched sample.
进一步地,在所述步骤S1中,所述晶体塑性本构方程包括主控方程,滑移流动准则方程以及背应力演化方程。Further, in the step S1, the crystal plasticity constitutive equation includes a master control equation, a slip flow criterion equation, and a back stress evolution equation.
进一步地,所述步骤S1包括:Further, the step S1 includes:
S11:建立晶体塑性本构方程中的所述几何不连续结构的材料的变形梯度F和变形速率梯度L的主控方程,所述几何不连续结构的材料的变形梯度F和变形速率梯度L的主控方程为:S11: Establish the main control equations of the deformation gradient F and the deformation rate gradient L of the material with the geometric discontinuous structure in the crystal plastic constitutive equation, and the deformation gradient F and the deformation rate gradient L of the material with the geometric discontinuous structure are The main control equation is:
F=F e·F pF=F e ·F p ,
L=L e+L pL=L e +L p ,
Figure PCTCN2020091262-appb-000001
Figure PCTCN2020091262-appb-000001
其中,F为总变形梯度,F e为弹性变形梯度,F p为非弹性变形梯度,L为变形速率梯度,L e为弹性变形速率梯度,L p为非弹性变形速率梯度,
Figure PCTCN2020091262-appb-000002
为第α滑移系的塑性滑移速率,s α为第α滑移系的滑移方向向量,m α为第α滑移系的法向方向向量;
Among them, F is the total deformation gradient, F e is the elastic deformation gradient, F p is the inelastic deformation gradient, L is the deformation rate gradient, Le is the elastic deformation rate gradient, L p is the inelastic deformation rate gradient,
Figure PCTCN2020091262-appb-000002
Is the plastic slip rate of the α-th slip system , s α is the slip direction vector of the α-th slip system, and m α is the normal direction vector of the α-th slip system;
S12:建立晶体塑性本构方程中的滑移流动准则方程,滑移流动准则方程为:S12: Establish the slip flow criterion equation in the crystal plasticity constitutive equation. The slip flow criterion equation is:
Figure PCTCN2020091262-appb-000003
Figure PCTCN2020091262-appb-000003
Figure PCTCN2020091262-appb-000004
Figure PCTCN2020091262-appb-000004
Figure PCTCN2020091262-appb-000005
Figure PCTCN2020091262-appb-000005
其中,
Figure PCTCN2020091262-appb-000006
为参考塑性滑移率,F 0为热激活自由能,k为玻尔兹曼常数,θ为绝对温度,τ α第α滑移系的分解剪切应力,σ为应力值;B α为第α滑移系的背应力,μ和μ 0分别是θ和0K时的剪切模量,τ 0、p、q为材料常数,S α为第α滑移系的滑移阻力,h s和d D分别为静态硬化和动态恢复模量,
Figure PCTCN2020091262-appb-000007
为第α滑移系的初始滑移阻力;
among them,
Figure PCTCN2020091262-appb-000006
Is the reference plastic slip rate, F 0 is the thermal activation free energy, k is Boltzmann’s constant, θ is the absolute temperature, τ α is the decomposed shear stress of the α-th slip system, and σ is the stress value; B α is the first The back stress of the α slip system, μ and μ 0 are the shear modulus at θ and 0K, respectively, τ 0 , p, q are the material constants, S α is the slip resistance of the α-th slip system, h s and d D is the static hardening and dynamic recovery modulus respectively,
Figure PCTCN2020091262-appb-000007
Is the initial slip resistance of the α-th slip system;
S13:建立晶体塑性本构方程中的背应力非弹性随动强化方程,所述背应力非弹性随动强化方程为:S13: Establish the back-stress inelastic follow-up strengthening equation in the crystal plastic constitutive equation, and the back-stress inelastic follow-up strengthening equation is:
Figure PCTCN2020091262-appb-000008
Figure PCTCN2020091262-appb-000008
Figure PCTCN2020091262-appb-000009
Figure PCTCN2020091262-appb-000009
其中,h B为背应力硬化常数,r D为滑移阻力相关动态回复系数,f c是内部变量相关的耦合参数,μ′ 0是在0K时的局部滑移剪切模量,λ为材料常数。 Among them, h B is the back-stress hardening constant, r D is the dynamic recovery coefficient related to slip resistance, f c is the coupling parameter related to internal variables, μ′ 0 is the local slip shear modulus at 0K, and λ is the material constant.
进一步地,在所述步骤S2中,所述单轴拉伸试验和单轴疲劳试验所采用的试样的形状与所述步骤S1中的第一ABAQUS有限元模型的形状相同。Further, in the step S2, the shape of the sample used in the uniaxial tensile test and the uniaxial fatigue test is the same as the shape of the first ABAQUS finite element model in the step S1.
进一步地,在所述步骤S3中,所述疲劳损伤计算模型根据所述步骤S1中的第一ABAQUS有限元模型和晶体塑性本构方程建立。Further, in the step S3, the fatigue damage calculation model is established according to the first ABAQUS finite element model and the crystal plasticity constitutive equation in the step S1.
进一步地,在所述步骤S3中,所述疲劳塑性滑移临界值P crit为: Further, in the step S3, the fatigue plastic slip critical value P crit is:
Figure PCTCN2020091262-appb-000010
Figure PCTCN2020091262-appb-000010
Figure PCTCN2020091262-appb-000011
Figure PCTCN2020091262-appb-000011
其中,L p为非弹性变形速率梯度,P crit为疲劳塑性滑移临界值。 Among them, L p is the inelastic deformation rate gradient, and P crit is the critical value of fatigue plastic slip.
进一步地,在所述步骤S4中,在模拟循环载荷的单轴疲劳试验时,其计算公式采用所述步骤S1中的用户子程序UMAT所定义的晶体塑性本构方程,且所施加的循环载荷与所述步骤S2单轴疲劳实验的载荷相同。Further, in the step S4, when simulating the uniaxial fatigue test of the cyclic load, the calculation formula adopts the crystal plastic constitutive equation defined by the user subroutine UMAT in the step S1, and the applied cyclic load The load is the same as that of the uniaxial fatigue test in step S2.
进一步地,所述步骤S4还包括:在建立所述几何不连续结构的第二ABAQUS有限元模型后,施加合理的边界条件和外部载荷,划分模型网格。Further, the step S4 further includes: after establishing the second ABAQUS finite element model of the geometric discontinuous structure, applying reasonable boundary conditions and external loads to divide the model mesh.
进一步地,在所述步骤S5中,所述裂纹萌生寿命为:Further, in the step S5, the crack initiation life is:
Figure PCTCN2020091262-appb-000012
Figure PCTCN2020091262-appb-000012
其中,N i为疲劳萌生寿命,P crit为疲劳塑性滑移临界值,P cyc为单周疲劳塑性滑移值。 Where, N i is the initiation of fatigue life, P crit plastic slip fatigue threshold, P cyc single cycle fatigue plastic slip value.
本发明利用疲劳塑性滑移临界值P crit作为疲劳指示因子,可以将微观尺度的参数用做损伤参量来进行寿命的评估,这种方法的好处在于微观尺度上的预测。不仅可以预测寿命,还能够获得每个循环周次中的塑性滑移损伤积累图,由此预测裂纹萌生的位置。 The present invention uses the fatigue plastic slip critical value P crit as the fatigue indicator, and can use micro-scale parameters as damage parameters to evaluate life. The advantage of this method lies in the prediction on the micro-scale. Not only can the life be predicted, but also the accumulation map of plastic slip damage in each cycle can be obtained, thereby predicting the location of crack initiation.
本发明的几何不连续结构的疲劳寿命预测方法所采用的用户子程序UMAT中的晶体塑性本构基于经典晶体塑性理论,能够得到几何不连续结构在疲劳载荷作用下的应力应变行为,且其采用的滑移流动准则方程是一种温度相关的幂指数型滑移流动准则,这样不仅可以模拟常温,也可以模拟高温,可以用来描述不同温度状态的力学行为,从而使得本发明的几何不连续结构的疲劳寿命预测方法能够预测高温下的结构寿命。The crystal plasticity constitutive in the user subroutine UMAT used in the fatigue life prediction method of the geometric discontinuous structure of the present invention is based on the classic crystal plasticity theory, and the stress and strain behavior of the geometric discontinuous structure under fatigue load can be obtained, and it adopts The slip flow criterion equation is a temperature-dependent power exponential slip flow criterion, which can simulate not only normal temperature but also high temperature, and can be used to describe the mechanical behavior of different temperature states, thereby making the geometric discontinuity of the present invention The fatigue life prediction method of structure can predict the structure life under high temperature.
本发明采用ABAQUS有限元模型,具有很强的直观性,可以直观地获 得几何不连续结构的裂纹萌生位置和并预测该位置的裂纹萌生寿命。The invention adopts the ABAQUS finite element model, which has strong intuitiveness, and can intuitively obtain the crack initiation position of the geometric discontinuous structure and predict the crack initiation life of the position.
附图说明Description of the drawings
图1为根据本发明的一个实施例的几何不连续结构的疲劳寿命预测方法的流程图;Fig. 1 is a flowchart of a method for predicting fatigue life of a geometrically discontinuous structure according to an embodiment of the present invention;
图2为根据本发明的一个实施例的几何不连续结构的疲劳寿命预测方法的第一ABAQUS有限元模型的示意图;2 is a schematic diagram of a first ABAQUS finite element model of a method for predicting fatigue life of a geometrically discontinuous structure according to an embodiment of the present invention;
图3为根据本发明的一个实施例的几何不连续结构的疲劳寿命预测方法的单轴拉伸试验和模拟曲线的拟合结果图;Fig. 3 is a graph of the uniaxial tensile test and simulation curve fitting results of the method for predicting the fatigue life of a geometric discontinuous structure according to an embodiment of the present invention;
图4为根据本发明的一个实施例的几何不连续结构的疲劳寿命预测方法的单轴疲劳试验的迟滞回线的数据和拟合曲线的拟合结果图;4 is a diagram of the hysteresis loop data of the uniaxial fatigue test and the fitting result diagram of the fitting curve of the fatigue life prediction method of the geometric discontinuous structure according to an embodiment of the present invention;
图5(a)-图5(h)为本发明的几何不连续结构的疲劳寿命预测方法的采用的不同缺口试样的有限元模型图,其中图5(a)-图5(h)示出了不同的缺口尺寸;Figures 5(a)-5(h) are the finite element model diagrams of different notched specimens used in the fatigue life prediction method of the geometric discontinuous structure of the present invention, wherein Figures 5(a)-5(h) show Different notch sizes;
图6为本发明的几何不连续结构的疲劳寿命预测方法的在不同缺口试样时,其不同循环周次累积的塑性应变线性增长轨迹图;Fig. 6 is a diagram showing the linear growth trajectory of plastic strain accumulated in different cycles of different notched specimens in the fatigue life prediction method of the geometric discontinuous structure of the present invention;
图7为不同缺口试样的寿命预测对比图;Figure 7 is a comparison diagram of life prediction for different notched specimens;
图8为本发明的几何不连续结构的疲劳寿命预测方法的不同缺口试样的寿命预测结果与实验验证结果的对比图;FIG. 8 is a comparison diagram of the life prediction results of different notched specimens and the experimental verification results of the fatigue life prediction method of the geometric discontinuous structure of the present invention;
图9为本发明的几何不连续结构的疲劳寿命预测方法预测的不同缺口长度与预测寿命之间的关系图;9 is a diagram of the relationship between different notch lengths and predicted life predicted by the fatigue life prediction method of the geometric discontinuous structure of the present invention;
图10为本发明的几何不连续结构的疲劳寿命预测方法预测的不同缺口面积与预测寿命之间的关系图。Fig. 10 is a diagram of the relationship between the different notch areas predicted by the fatigue life prediction method of the geometric discontinuous structure of the present invention and the predicted life.
具体实施方式Detailed ways
下面根据附图1-9,给出本发明的较佳实施例,并予以详细描述,使能更好地理解本发明的功能、特点。Hereinafter, preferred embodiments of the present invention are given and described in detail according to the attached drawings 1-9, so that the functions and characteristics of the present invention can be better understood.
请参阅图1为本发明公开的一种几何不连续结构的疲劳寿命预测方法,其包括以下步骤:Please refer to FIG. 1 for a method for predicting fatigue life of a geometrically discontinuous structure disclosed in the present invention, which includes the following steps:
S1:建立一个几何连续(即不含缺口)且包含所述几何不连续结构的 材料的一定数量的晶粒的第一ABAQUS有限元模型,其中,所述晶粒的数量通常为多个,并通过用户子程序UMAT定义该材料在循环载荷的单轴疲劳试验的过程中的晶体塑性本构方程,以此得到所述材料在给定的循环载荷条件下的应力应变关系;S1: Establish a first ABAQUS finite element model of a certain number of crystal grains that are geometrically continuous (that is, without gaps) and include the material with the geometric discontinuous structure, where the number of the crystal grains is usually multiple, and Define the crystal plastic constitutive equation of the material during the uniaxial fatigue test under cyclic loading through the user subroutine UMAT, so as to obtain the stress-strain relationship of the material under the given cyclic loading condition;
第一ABAQUS有限元模型是指采用有限元软件ABAQUS建模的模型,其形状如图2所示,用来描述所述几何不连续结构的材料的微观结构信息。晶体塑性本构方程包括主控方程,滑移流动准则方程以及背应力演化方程等(即下文所述的公式1到11这些模型公式),用来描述所述几何不连续结构的材料的应力应变关系,并用于嵌入第一ABAQUS有限元模型以进行有限元的计算。应力应变关系包括弹性部分和塑性部分,其塑性部分利用所述晶体塑性本构方程计算得出。The first ABAQUS finite element model refers to a model modeled by the finite element software ABAQUS, the shape of which is shown in FIG. 2, and is used to describe the microstructure information of the material with the geometric discontinuous structure. The crystal plastic constitutive equations include master control equations, slip flow criterion equations, and back stress evolution equations (ie formulas 1 to 11 described below), which are used to describe the stress and strain of the material with the geometric discontinuous structure Relationship and used to embed the first ABAQUS finite element model for finite element calculations. The stress-strain relationship includes an elastic part and a plastic part, and the plastic part is calculated using the crystal plastic constitutive equation.
其中,步骤S1进一步包括步骤:Wherein, step S1 further includes the steps:
S11:建立晶体塑性本构方程中的所述几何不连续结构的材料的变形梯度F和变形速率梯度L的主控方程。S11: Establish a master control equation for the deformation gradient F and the deformation rate gradient L of the material with the geometric discontinuous structure in the crystal plasticity constitutive equation.
其中,所述几何不连续结构的材料的变形梯度F和变形速率梯度L的主控方程为:Wherein, the main control equations of the deformation gradient F and the deformation rate gradient L of the material with the geometric discontinuous structure are:
F=F e·F p         (1); F=F e ·F p (1);
L=L e+L p         (2); L=L e +L p (2);
Figure PCTCN2020091262-appb-000013
Figure PCTCN2020091262-appb-000013
其中,F为总变形梯度,F e为弹性变形梯度,F p为非弹性变形梯度,L为变形速率梯度,L e为弹性变形速率梯度,L p为非弹性变形速率梯度,
Figure PCTCN2020091262-appb-000014
为第α滑移系的塑性滑移速率,s α为第α滑移系的滑移方向向量,m α为第α滑移系的法向方向向量;
Among them, F is the total deformation gradient, F e is the elastic deformation gradient, F p is the inelastic deformation gradient, L is the deformation rate gradient, Le is the elastic deformation rate gradient, L p is the inelastic deformation rate gradient,
Figure PCTCN2020091262-appb-000014
Is the plastic slip rate of the α-th slip system , s α is the slip direction vector of the α-th slip system, and m α is the normal direction vector of the α-th slip system;
S12:建立晶体塑性本构方程中的滑移流动准则方程,滑移流动准则方程包括:S12: Establish the slip flow criterion equation in the crystal plastic constitutive equation. The slip flow criterion equation includes:
Figure PCTCN2020091262-appb-000015
Figure PCTCN2020091262-appb-000015
Figure PCTCN2020091262-appb-000016
Figure PCTCN2020091262-appb-000016
Figure PCTCN2020091262-appb-000017
Figure PCTCN2020091262-appb-000017
其中,
Figure PCTCN2020091262-appb-000018
为第α滑移系的塑性滑移速率,
Figure PCTCN2020091262-appb-000019
为参考塑性滑移率,F 0为热激活自由能,单位为kJ·mol -1,k为玻尔兹曼常数,θ(T)为绝对温度,τ α第α滑移系的分解剪切应力,单位为MPa,演化方程如公式(5)所示,σ为应力值,单位为MPa;B α为第α滑移系的背应力,单位为MPa,μ和μ 0分别是θ和0K时的剪切模量,单位均为GPa,τ 0、p、q为材料常数,τ 0的单位为MPa。运算符号<>表示:当x>0时,<x>=x;当x≤0时,<x>=0。S α为第α滑移系的滑移阻力,单位为MPa。其演化方程如公式(6)所示,h s和d D分别为静态硬化和动态恢复模量,单位均为MPa,
Figure PCTCN2020091262-appb-000020
为第α滑移系的初始滑移阻力,单位为MPa。
among them,
Figure PCTCN2020091262-appb-000018
Is the plastic slip rate of the α-th slip system,
Figure PCTCN2020091262-appb-000019
Is the reference plastic slip rate, F 0 is the thermal activation free energy, the unit is kJ·mol -1 , k is Boltzmann's constant, θ(T) is the absolute temperature, τ α is the decomposition shear of the α-th slip system Stress, the unit is MPa, the evolution equation is shown in formula (5), σ is the stress value, the unit is MPa; B α is the back stress of the α-th slip system, the unit is MPa, μ and μ 0 are respectively θ and 0K The unit of shear modulus at time is GPa, τ 0 , p, q are material constants, and the unit of τ 0 is MPa. The operation symbol <> means: when x>0, <x>=x; when x≤0, <x>=0. S α is the slip resistance of the α-th slip system, in MPa. Its evolution equation is shown in formula (6), h s and d D are static hardening and dynamic recovery modulus, respectively, in units of MPa,
Figure PCTCN2020091262-appb-000020
Is the initial slip resistance of the α-th slip system, in MPa.
由于本发明的几何不连续结构的疲劳寿命预测方法所采用的晶体塑性本构方程中的滑移流动准则方程是一种幂指数型滑移流动准则,与传统幂函数型相比,嵌入了热激活能等温度相关参数,可以模拟不同温度的材料力学行为。Since the slip flow criterion equation in the crystal plastic constitutive equation used in the fatigue life prediction method of the geometric discontinuous structure of the present invention is a power exponential slip flow criterion, compared with the traditional power function type, heat is embedded Temperature-related parameters such as activation energy can simulate the mechanical behavior of materials at different temperatures.
S13:建立晶体塑性本构方程中的背应力非弹性随动强化方程,其中,背应力非弹性随动强化方程为:S13: Establish the back-stress inelastic follow-up strengthening equation in the crystal plastic constitutive equation, where the back-stress inelastic follow-up strengthening equation is:
Figure PCTCN2020091262-appb-000021
Figure PCTCN2020091262-appb-000021
Figure PCTCN2020091262-appb-000022
Figure PCTCN2020091262-appb-000022
其中,h B为背应力硬化常数,单位为MPa,r D为滑移阻力相关动态回复系数,演化方程如公式(8)所示,f c是内部变量相关的耦合参数,μ′ 0是在0K时的局部滑移剪切模量,单位为GPa,λ为材料常数。 Among them, h B is the back stress hardening constant, the unit is MPa, r D is the dynamic recovery coefficient related to slip resistance, the evolution equation is shown in formula (8), f c is the coupling parameter related to internal variables, and μ′ 0 is The local slip shear modulus at 0K, the unit is GPa, and λ is the material constant.
本发明的几何不连续结构的疲劳寿命预测方法所采用了背应力非弹性 随动强化方程,由此考虑了温度效应。The fatigue life prediction method of the geometric discontinuous structure of the present invention adopts the back stress inelastic follow-up strengthening equation, thereby taking into account the temperature effect.
S2:对所述几何不连续结构的材料在同一温度下进行单轴拉伸试验以及不同应变幅的单轴疲劳试验,得到拉伸曲线和迟滞回线。在本实施例中,所使用的温度都是室温,但是本发明的方法也可以应用于材料的各种服役温度。S2: Perform a uniaxial tensile test and a uniaxial fatigue test with different strain amplitudes on the material with the geometric discontinuous structure at the same temperature to obtain a tensile curve and a hysteresis loop. In this embodiment, the temperatures used are all room temperature, but the method of the present invention can also be applied to various service temperatures of materials.
其中,所述单轴拉伸试验和单轴疲劳试验所采用的试样的形状与所述步骤S1中的第一ABAQUS有限元模型的形状相同。Wherein, the shape of the sample used in the uniaxial tensile test and the uniaxial fatigue test is the same as the shape of the first ABAQUS finite element model in step S1.
S3:建立疲劳损伤计算模型,通过试参法拟合获得所述第一ABAQUS有限元模型的拉伸曲线和迟滞回线,直至拟合获得的拉伸曲线和迟滞回线与所述步骤S2中的试验所得的拉伸曲线和迟滞回线有较好的拟合程度,进而获取晶体塑性本构方程所需的材料参数
Figure PCTCN2020091262-appb-000023
F 0,p,q,τ 0,s 0,h s,d D0,μ′ 0,h B,f C,μ,λ和疲劳塑性滑移临界值P crit。其中,疲劳塑性滑移临界值P crit是相对于现有技术新增的参数。
S3: Establish a fatigue damage calculation model, and obtain the tensile curve and hysteresis loop of the first ABAQUS finite element model through trial-parameter fitting, until the obtained tensile curve and hysteresis loop are the same as in step S2 The tensile curve and hysteresis loop obtained from the test have a good degree of fit, and then the material parameters required for the crystal plasticity constitutive equation can be obtained
Figure PCTCN2020091262-appb-000023
F 0 ,p,q,τ 0 ,s 0 ,h s ,d D0 ,μ′ 0 ,h B ,f C ,μ,λ and the critical fatigue plastic slip value P crit . Among them, the fatigue plastic slip critical value P crit is a new parameter relative to the prior art.
其中,所述疲劳损伤计算模型根据所述步骤S1中的第一ABAQUS有限元模型和晶体塑性本构方程建立。Wherein, the fatigue damage calculation model is established according to the first ABAQUS finite element model and the crystal plasticity constitutive equation in the step S1.
疲劳塑性滑移临界值P crit的计算公式如下: The calculation formula of fatigue plastic slip critical value P crit is as follows:
Figure PCTCN2020091262-appb-000024
Figure PCTCN2020091262-appb-000024
Figure PCTCN2020091262-appb-000025
Figure PCTCN2020091262-appb-000025
其中,L p为非弹性变形速率梯度,P crit为疲劳塑性滑移临界值,
Figure PCTCN2020091262-appb-000026
为疲劳塑性滑移的变化率。
Among them, L p is the inelastic deformation rate gradient, P crit is the critical value of fatigue plastic slip,
Figure PCTCN2020091262-appb-000026
Is the rate of change of fatigue plastic slip.
由于上述步骤S1的第一ABAQUS有限元模型是几何连续的,即不含缺口的,其用于校订参数。因为该第一ABAQUS有限元模型可以与步骤S2中的拉伸曲线和迟滞回线进行拟合,所以我们通过不含缺口的第一ABAQUS有限元模型来与实验进行拟合从而确定参数。Since the first ABAQUS finite element model of step S1 is geometrically continuous, that is, it does not contain gaps, it is used for parameter correction. Because the first ABAQUS finite element model can be fitted with the stretch curve and hysteresis loop in step S2, we use the first ABAQUS finite element model without gaps to fit the experiment to determine the parameters.
S4:建立所述几何不连续结构(即,含缺口)的第二ABAQUS有限元模型,施加合理的边界条件和外部载荷,划分模型网格,并结合所述步骤S1的用户子程序UMAT和所述步骤S3的材料参数和疲劳塑性滑移临界值P crit, 采用ABAQUS软件来模拟循环载荷的单轴疲劳试验,得到每个循环周次的(每个积分点)的应力应变关系和单周疲劳塑性滑移值,单周疲劳塑性滑移值的计算也是利用公式(9)和(10)。所述几何不连续结构的模型形状和缺口可根据工程实际情况而改变,由于其为本发明的寿命预测对象,所以建立含缺口的第二有限元模型来预测寿命。 S4: Establish a second ABAQUS finite element model of the geometric discontinuous structure (that is, including gaps), apply reasonable boundary conditions and external loads, divide the model mesh, and combine the user subroutine UMAT of step S1 with all The material parameters and fatigue plastic slip critical value P crit of step S3 are described. The ABAQUS software is used to simulate the uniaxial fatigue test of cyclic loading, and the stress-strain relationship and single-cycle fatigue of each cycle (each integration point) are obtained. The calculation of plastic slip value and single cycle fatigue plastic slip value also use formulas (9) and (10). The model shape and gap of the geometric discontinuous structure can be changed according to actual engineering conditions. Since it is the life prediction object of the present invention, a second finite element model with gaps is established to predict the life.
其中,所述循环周次的总数可以为一直到疲劳断裂时的总的循环周次。在模拟循环载荷的单轴疲劳试验时,其计算公式采用所述步骤S1中的用户子程序UMAT所定义的晶体塑性本构方程,且所施加的循环载荷与所述步骤S2单轴疲劳实验的载荷相同,由此来计算每个周次的演化。由此,可以获得单周疲劳塑性滑移值和如图6所示的每个周次的塑性滑移的演化过程。Wherein, the total number of cycle cycles may be the total cycle cycles up to the time of fatigue fracture. When simulating the uniaxial fatigue test under cyclic load, the calculation formula adopts the crystal plasticity constitutive equation defined by the user subroutine UMAT in step S1, and the applied cyclic load is the same as that of the uniaxial fatigue test in step S2. The load is the same, and the evolution of each cycle is calculated from this. As a result, the single-cycle fatigue plastic slip value and the evolution process of plastic slip per cycle as shown in Fig. 6 can be obtained.
S5:结合所述步骤S3的疲劳塑性滑移临界值和所述步骤S4的单周疲劳塑性滑移值,计算得到缺口试样的裂纹萌生寿命。S5: Combining the critical fatigue plastic slip value of step S3 and the single-cycle fatigue plastic slip value of step S4, calculate the crack initiation life of the notched sample.
其中,所述裂纹萌生寿命为:Wherein, the crack initiation life is:
Figure PCTCN2020091262-appb-000027
Figure PCTCN2020091262-appb-000027
其中,N i为裂纹萌生寿命,P crit为疲劳塑性滑移临界值,P cyc为单周疲劳塑性滑移值。 Where, N i is the crack initiation life, P crit plastic slip fatigue threshold, P cyc single cycle fatigue plastic slip value.
实验结果Experimental results
下面采用本发明提供的几何不连续结构的疲劳寿命预测方法对不同缺口试样,并采用实验的萌生寿命信息来验证本发明的有效性。其中,缺口试样的材料为镍基GH4169超合金,疲劳试验在常温空气环境下进行。试样两端施加的外载和为整体的应力控制,由于单边缺口试样的几何不连续性的影响,其缺口的最薄弱的部位处于多轴应力应变状态。In the following, the fatigue life prediction method of geometric discontinuous structure provided by the present invention is used to verify the effectiveness of the present invention for different notched specimens, and the initiation life information of the experiment is used. Among them, the material of the notched sample is nickel-based GH4169 superalloy, and the fatigue test is carried out in an air environment at room temperature. The external load applied at both ends of the specimen is the overall stress control. Due to the geometric discontinuity of the unilateral notch specimen, the weakest part of the notch is in a multiaxial stress-strain state.
本发明的几何不连续结构的疲劳寿命预测方法需要对同样材质的不含缺口的试样进行常温空气环境下的单轴拉伸试验以及该环境下不同应变幅的单轴疲劳试验,获得的试验结果用于在本发明的几何不连续结构的疲劳寿命预测方法的步骤S2中确定公式(1)~(8)以及(11)的晶体塑性本构方程所需的材料参数。首先建立如图2所示的不含缺口的ABAQUS模型,通过试参法调整单轴拉伸和疲劳试验的模拟结果,使之与单轴拉伸和疲劳试验数据 能够较好地吻合,拟合结果如图3和图4所示。其中,拟合结果为:
Figure PCTCN2020091262-appb-000028
F 0=295kJ·mol -1,θ=293K,p=0.31,q=1.8,τ 0=810MPa,s 0=340MPa,h s=513MPa,d D=6030MPa,μ 0=192GPa,μ′ 0=72.3GPa,h B=540MPa,f C=0.41,μ=73.65GPa,λ=0.85。
The fatigue life prediction method of the geometric discontinuous structure of the present invention requires uniaxial tensile test under normal temperature air environment and uniaxial fatigue test with different strain amplitudes on samples without notches of the same material. The obtained test The result is used to determine the material parameters required by the crystal plastic constitutive equations of formulas (1) to (8) and (11) in step S2 of the fatigue life prediction method of the geometric discontinuous structure of the present invention. First, establish the ABAQUS model without notches as shown in Figure 2, and adjust the simulation results of uniaxial tensile and fatigue tests by the trial parameter method, so that it can be better matched with the uniaxial tensile and fatigue test data. The results are shown in Figure 3 and Figure 4. Among them, the fitting result is:
Figure PCTCN2020091262-appb-000028
F 0 =295kJ·mol -1 , θ = 293K, p = 0.31, q = 1.8, τ 0 =810MPa, s 0 =340MPa, h s =513MPa, d D =6030MPa, μ 0 =192GPa, μ′ 0 = 72.3GPa, h B =540 MPa, f C =0.41, μ=73.65GPa, λ=0.85.
通过采用本发明的几何不连续结构的疲劳寿命预测方法,可以根据拟合结果,确定疲劳塑性滑移临界值P crit,然后对含不同缺口材料进行寿命预测。 By adopting the fatigue life prediction method of the geometric discontinuous structure of the present invention, the critical value P crit of fatigue plastic slip can be determined according to the fitting result, and then the life prediction of materials with different notches can be carried out.
图5(a)-图5(h)给出了不同缺口试样的ABAQUS模型图。模型大小相同,改变了不同的缺口尺寸,其中a表示缺口的长,b表示缺口的宽。图6给出了不同缺口试样的每个循环周次的疲劳累积塑性应变轨迹图。可以看出,缺口尺寸较大时,累积塑性滑移也较大。此外,塑性累积是呈线性的,因此可以用上文所述公式(11)来计算不同试样的疲劳萌生寿命。图7给出了不同缺口试样的寿命预测图。可以看出,本发明的几何不连续结构的疲劳寿命预测方法通过累积塑性滑移来预测萌生寿命的结果,与实验的结果较为接近,在2倍误差带范围内,因此,证明了此数值模拟方法的具有较高的可靠性。此外,在数值模拟的结果中,还能预测裂纹萌生的位置。裂纹萌生主要集中在两个区域,一个是缺口根部应力集中区,这是由于在缺口根部是疲劳过程中的潜在危险点,应力集中效应比较明显;一个是在远离根部的位置,此区域的裂纹萌生主要是由于局部晶粒的塑性变形较大所导致的。Figure 5 (a)-Figure 5 (h) show the ABAQUS model diagrams of different notched samples. The size of the model is the same, and different gap sizes are changed, where a represents the length of the gap and b represents the width of the gap. Figure 6 shows the fatigue cumulative plastic strain trajectory diagram for each cycle of different notched specimens. It can be seen that when the size of the gap is larger, the cumulative plastic slip is also larger. In addition, plastic accumulation is linear, so the above formula (11) can be used to calculate the fatigue initiation life of different specimens. Figure 7 shows the life prediction diagrams of different notched specimens. It can be seen that the fatigue life prediction method of the geometric discontinuous structure of the present invention uses cumulative plastic slip to predict the result of the initiation life, which is relatively close to the experimental result and within the range of 2 times the error band. Therefore, this numerical simulation is proved The method has high reliability. In addition, in the results of the numerical simulation, the location of crack initiation can also be predicted. Crack initiation is mainly concentrated in two areas, one is the stress concentration area at the root of the notch. This is because the root of the notch is a potential dangerous point in the fatigue process, and the stress concentration effect is more obvious; the other is at a location far away from the root, where the cracks are located in this area. The initiation is mainly caused by the large plastic deformation of local grains.
在采用本发明的几何不连续结构的疲劳寿命预测方法所得到的上述预测结果的基础上,下面建立更多几何不连续结构的模型(相同尺寸但是晶粒取向不同),并通过实验来验证该方法的可行性和适用性。On the basis of the above-mentioned prediction results obtained by the fatigue life prediction method of the geometric discontinuous structure of the present invention, more models of the geometric discontinuous structure (the same size but different grain orientation) are established below, and the experiments are used to verify this The feasibility and applicability of the method.
图8给出了不同模型的寿命预测与实验结果的对比图,从图中可以看出,采用本发明得到的所有预测结果与实验结果的寿命对比,均在2倍误差带范围之内,证明此数值模拟方法具有较高的可靠性和稳定性。此外,针对不同缺口长度和缺口面积进行分析发现,寿命与缺口长度和缺口面积有很大的关系。图9给出了不同缺口长度的寿命对比图,从图中可以看出,随着缺口长度的增加,疲劳寿命是逐渐降低的,此外,在长度达到一定的数值以后,寿命会达到一个平台,后期缺口的长度会影响较小。图10给出了不同缺口面积的寿命对比图,从图中可以看出,随着缺口面积的增加,疲劳寿命也是逐 渐减小的,在缺口面积增加后,也会出现平台现象。而且,缺口面积和疲劳寿命存在一定的演化关系:Figure 8 shows the comparison diagram of the life prediction of different models and the experimental results. It can be seen from the figure that the life comparison of all the prediction results obtained by the present invention and the experimental results are within the range of 2 times the error band, which proves This numerical simulation method has high reliability and stability. In addition, the analysis of different notch length and notch area reveals that the life span has a great relationship with notch length and notch area. Figure 9 shows the life comparison diagram of different notch lengths. It can be seen from the figure that as the length of the notch increases, the fatigue life gradually decreases. In addition, after the length reaches a certain value, the life will reach a plateau. The length of the gap in the later period will have a smaller effect. Figure 10 shows the life comparison chart of different notch areas. It can be seen from the figure that as the notch area increases, the fatigue life gradually decreases. After the notch area increases, the plateau phenomenon will also appear. Moreover, there is a certain evolutionary relationship between notch area and fatigue life:
Figure PCTCN2020091262-appb-000029
Figure PCTCN2020091262-appb-000029
其中A为缺口面积,N i为疲劳寿命。 Wherein A is the area of the notch, N i is the fatigue life.
以上记载的,仅为本发明的较佳实施例,并非用以限定本发明的范围,本发明的上述实施例还可以做出各种变化。即凡是依据本发明申请的权利要求书及说明书内容所作的简单、等效变化与修饰,皆落入本发明专利的权利要求保护范围。The foregoing descriptions are only preferred embodiments of the present invention, and are not used to limit the scope of the present invention. Various changes can be made to the foregoing embodiments of the present invention. That is to say, all simple and equivalent changes and modifications made in accordance with the claims of the present invention and the contents of the description fall into the protection scope of the patent of the present invention.

Claims (9)

  1. 一种几何不连续结构的疲劳寿命预测方法,其特征在于,其包括以下步骤:A method for predicting the fatigue life of a geometrically discontinuous structure, which is characterized in that it comprises the following steps:
    S1:建立一个几何连续且包含所述几何不连续结构的材料的多个晶粒的第一ABAQUS有限元模型,并通过用户子程序UMAT定义所述材料在循环载荷的单轴疲劳试验的过程中的晶体塑性本构方程,以此得到所述材料在给定的循环载荷条件下的应力应变关系;S1: Establish a geometrically continuous first ABAQUS finite element model containing multiple crystal grains of the material with the geometric discontinuous structure, and define the material during the cyclic load uniaxial fatigue test through the user subroutine UMAT The crystal plasticity constitutive equation of, to obtain the stress-strain relationship of the material under given cyclic loading conditions;
    S2:对所述几何不连续结构的材料在同一温度下进行单轴拉伸试验以及不同应变幅的单轴疲劳试验,得到拉伸曲线和迟滞回线;S2: Perform uniaxial tensile test and uniaxial fatigue test with different strain amplitudes on the material with the geometric discontinuous structure at the same temperature to obtain the tensile curve and hysteresis loop;
    S3:建立疲劳损伤计算模型,通过试参法拟合获得所述第一ABAQUS有限元模型的拉伸曲线和迟滞回线,进而获取所述晶体塑性本构方程所需的材料参数和疲劳塑性滑移临界值;S3: Establish a fatigue damage calculation model, and obtain the tensile curve and hysteresis loop of the first ABAQUS finite element model through trial-parameter fitting, and then obtain the material parameters and fatigue plastic slip required by the crystal plastic constitutive equation Shift critical value;
    S4:建立所述几何不连续结构的第二ABAQUS有限元模型,并结合所述步骤S1的用户子程序UMAT和所述步骤S3的材料参数和疲劳塑性滑移临界值,采用ABAQUS软件来模拟循环载荷的单轴疲劳试验,得到每个循环周次的应力应变关系和单周疲劳塑性滑移值;S4: Establish a second ABAQUS finite element model of the geometric discontinuous structure, and combine the user subroutine UMAT of step S1 with the material parameters and fatigue plastic slip critical value of step S3, and use ABAQUS software to simulate the cycle Load uniaxial fatigue test to obtain the stress-strain relationship and single-cycle fatigue plastic slip value for each cycle;
    S5:结合所述步骤S3的疲劳塑性滑移临界值和所述步骤S4的单周疲劳塑性滑移值,计算得到缺口试样的裂纹萌生寿命。S5: Combining the critical fatigue plastic slip value of step S3 and the single-cycle fatigue plastic slip value of step S4, calculate the crack initiation life of the notched sample.
  2. 根据权利要求1所述的几何不连续结构的疲劳寿命预测方法,其特征在于,在所述步骤S1中,所述晶体塑性本构方程包括主控方程,滑移流动准则方程以及背应力演化方程。The method for predicting the fatigue life of a geometric discontinuous structure according to claim 1, wherein in the step S1, the crystal plastic constitutive equation includes a master control equation, a slip flow criterion equation, and a back stress evolution equation .
  3. 根据权利要求2所述的几何不连续结构的疲劳寿命预测方法,其特征在于,所述步骤S1包括:The method for predicting the fatigue life of a geometrically discontinuous structure according to claim 2, wherein the step S1 comprises:
    S11:建立晶体塑性本构方程中的所述几何不连续结构的材料的变形梯度F和变形速率梯度L的主控方程,所述几何不连续结构的材料的变形梯度F和变形速率梯度L的主控方程为:S11: Establish the main control equations of the deformation gradient F and the deformation rate gradient L of the material with the geometric discontinuous structure in the crystal plastic constitutive equation, and the deformation gradient F and the deformation rate gradient L of the material with the geometric discontinuous structure are The main control equation is:
    F=F e·F pF=F e ·F p ,
    L=L e+L pL=L e +L p ,
    Figure PCTCN2020091262-appb-100001
    Figure PCTCN2020091262-appb-100001
    其中,F为总变形梯度,F e为弹性变形梯度,F p为非弹性变形梯度,L为变形速率梯度,L e为弹性变形速率梯度,L p为非弹性变形速率梯度,
    Figure PCTCN2020091262-appb-100002
    为第α滑移系的塑性滑移速率,s α为第α滑移系的滑移方向向量,m α为第α滑移系的法向方向向量;
    Among them, F is the total deformation gradient, F e is the elastic deformation gradient, F p is the inelastic deformation gradient, L is the deformation rate gradient, Le is the elastic deformation rate gradient, L p is the inelastic deformation rate gradient,
    Figure PCTCN2020091262-appb-100002
    Is the plastic slip rate of the α-th slip system , s α is the slip direction vector of the α-th slip system, and m α is the normal direction vector of the α-th slip system;
    S12:建立晶体塑性本构方程中的滑移流动准则方程,滑移流动准则方程为:S12: Establish the slip flow criterion equation in the crystal plasticity constitutive equation. The slip flow criterion equation is:
    Figure PCTCN2020091262-appb-100003
    Figure PCTCN2020091262-appb-100003
    Figure PCTCN2020091262-appb-100004
    Figure PCTCN2020091262-appb-100004
    Figure PCTCN2020091262-appb-100005
    Figure PCTCN2020091262-appb-100005
    其中,
    Figure PCTCN2020091262-appb-100006
    为参考塑性滑移率,F 0为热激活自由能,k为玻尔兹曼常数,θ为绝对温度,τ α第α滑移系的分解剪切应力,σ为应力值;B α为第α滑移系的背应力,μ和μ 0分别是θ和0K时的剪切模量,τ 0、p、q为材料常数,S α为第α滑移系的滑移阻力,h s和d D分别为静态硬化和动态恢复模量,
    Figure PCTCN2020091262-appb-100007
    为第α滑移系的初始滑移阻力;
    among them,
    Figure PCTCN2020091262-appb-100006
    Is the reference plastic slip rate, F 0 is the thermal activation free energy, k is Boltzmann’s constant, θ is the absolute temperature, τ α is the decomposed shear stress of the α-th slip system, and σ is the stress value; B α is the first The back stress of the α slip system, μ and μ 0 are the shear modulus at θ and 0K, respectively, τ 0 , p, q are the material constants, S α is the slip resistance of the α-th slip system, h s and d D is the static hardening and dynamic recovery modulus respectively,
    Figure PCTCN2020091262-appb-100007
    Is the initial slip resistance of the α-th slip system;
    S13:建立晶体塑性本构方程中的背应力非弹性随动强化方程,所述背应力非弹性随动强化方程为:S13: Establish the back-stress inelastic follow-up strengthening equation in the crystal plastic constitutive equation, and the back-stress inelastic follow-up strengthening equation is:
    Figure PCTCN2020091262-appb-100008
    Figure PCTCN2020091262-appb-100008
    Figure PCTCN2020091262-appb-100009
    Figure PCTCN2020091262-appb-100009
    其中,h B为背应力硬化常数,r D为滑移阻力相关动态回复系数,f c是内部变量相关的耦合参数,μ′ 0是在0K时的局部滑移剪切模量,λ为材料常数。 Among them, h B is the back-stress hardening constant, r D is the dynamic recovery coefficient related to slip resistance, f c is the coupling parameter related to internal variables, μ′ 0 is the local slip shear modulus at 0K, and λ is the material constant.
  4. 根据权利要求1所述的几何不连续结构的疲劳寿命预测方法,其特征在于,在所述步骤S2中,所述单轴拉伸试验和单轴疲劳试验所采用的试样的 形状与所述步骤S1中的第一ABAQUS有限元模型的形状相同。The method for predicting the fatigue life of a geometric discontinuous structure according to claim 1, wherein in the step S2, the shape of the sample used in the uniaxial tensile test and the uniaxial fatigue test is the same as that of the The shape of the first ABAQUS finite element model in step S1 is the same.
  5. 根据权利要求1所述的几何不连续结构的疲劳寿命预测方法,其特征在于,在所述步骤S3中,所述疲劳损伤计算模型根据所述步骤S1中的第一ABAQUS有限元模型和晶体塑性本构方程建立。The method for predicting the fatigue life of a geometric discontinuous structure according to claim 1, wherein in the step S3, the fatigue damage calculation model is based on the first ABAQUS finite element model and the crystal plasticity in the step S1 The constitutive equation is established.
  6. 根据权利要求1所述的几何不连续结构的疲劳寿命预测方法,其特征在于,在所述步骤S3中,所述疲劳塑性滑移临界值P crit为: The method for predicting the fatigue life of a geometrically discontinuous structure according to claim 1, wherein in the step S3, the fatigue plastic slip critical value P crit is:
    Figure PCTCN2020091262-appb-100010
    Figure PCTCN2020091262-appb-100010
    Figure PCTCN2020091262-appb-100011
    Figure PCTCN2020091262-appb-100011
    其中,L p为非弹性变形速率梯度,P crit为疲劳塑性滑移临界值。 Among them, L p is the inelastic deformation rate gradient, and P crit is the critical value of fatigue plastic slip.
  7. 根据权利要求1所述的几何不连续结构的疲劳寿命预测方法,其特征在于,在所述步骤S4中,在模拟循环载荷的单轴疲劳试验时,其计算公式采用所述步骤S1中的用户子程序UMAT所定义的晶体塑性本构方程,且所施加的循环载荷与所述步骤S2中的单轴疲劳实验的载荷相同。The method for predicting the fatigue life of a geometric discontinuous structure according to claim 1, characterized in that, in the step S4, when simulating the uniaxial fatigue test of cyclic load, the calculation formula adopts the user in the step S1 The crystal plasticity constitutive equation defined by the subroutine UMAT, and the applied cyclic load is the same as the load of the uniaxial fatigue test in step S2.
  8. 根据权利要求1所述的几何不连续结构的疲劳寿命预测方法,其特征在于,所述步骤S4还包括:在建立所述几何不连续结构的第二ABAQUS有限元模型后,施加合理的边界条件和外部载荷,划分模型网格。The fatigue life prediction method of the geometric discontinuous structure according to claim 1, wherein the step S4 further comprises: after establishing a second ABAQUS finite element model of the geometric discontinuous structure, applying reasonable boundary conditions And external loads, and mesh the model.
  9. 根据权利要求1所述的几何不连续结构的疲劳寿命预测方法,其特征在于,在所述步骤S5中,所述裂纹萌生寿命为:The method for predicting the fatigue life of a geometrically discontinuous structure according to claim 1, wherein, in the step S5, the crack initiation life is:
    Figure PCTCN2020091262-appb-100012
    Figure PCTCN2020091262-appb-100012
    其中,N i为疲劳萌生寿命,P crit为疲劳塑性滑移临界值,P cyc为单周疲劳塑性滑移值。 Where, N i is the initiation of fatigue life, P crit plastic slip fatigue threshold, P cyc single cycle fatigue plastic slip value.
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