CN115841857A - Method for predicting service life of internal fatigue failure of metal material - Google Patents

Method for predicting service life of internal fatigue failure of metal material Download PDF

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CN115841857A
CN115841857A CN202211555386.3A CN202211555386A CN115841857A CN 115841857 A CN115841857 A CN 115841857A CN 202211555386 A CN202211555386 A CN 202211555386A CN 115841857 A CN115841857 A CN 115841857A
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life
metal material
crack
crack initiation
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孙锐
张文
白润
刘辉
白伟
周永康
王峰
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Northwest Institute for Non Ferrous Metal Research
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Abstract

本发明公开了一种金属材料内部疲劳失效的寿命预测方法,包括:一、获取加载恒定载荷条件下金属材料的应力‑寿命拟合公式;二、获取初始吉布斯自由能变方程;三、获取周期性载荷加载条件下的塑性应变能密度;四、修正初始吉布斯自由能变方程中的裂纹表面能;五、预估裂纹萌生寿命;六、验证获取的裂纹萌生寿命精度。本发明通过建立基于吉布斯自由能变与内部裂纹萌生时能量演化的关系,随后结合晶体塑性有限元计算循环加载条件下的塑性应变能密度,进而基于能效因子评估对初始吉布斯自由能变方程进行修正,建立细观内部疲劳裂纹萌生寿命预测模型,对金属材料的疲劳寿命进行预估和验证,满足了机械结构环境‑高性能‑长寿命设计要求。

Figure 202211555386

The invention discloses a life prediction method for internal fatigue failure of metal materials, comprising: 1. Obtaining the stress-life fitting formula of the metal material under the condition of constant load; 2. Obtaining the initial Gibbs free energy change equation; 3. Obtain the plastic strain energy density under cyclic loading conditions; 4. Correct the crack surface energy in the initial Gibbs free energy change equation; 5. Estimate the crack initiation life; 6. Verify the accuracy of the obtained crack initiation life. The present invention establishes the relationship between Gibbs free energy change and internal crack initiation energy evolution, and then calculates the plastic strain energy density under cyclic loading conditions in combination with crystal plastic finite elements, and then evaluates the initial Gibbs free energy based on the energy efficiency factor. The variable equation is corrected, and the mesoscopic internal fatigue crack initiation life prediction model is established to predict and verify the fatigue life of metal materials, which meets the design requirements of mechanical structure environment-high performance-long life.

Figure 202211555386

Description

一种金属材料内部疲劳失效的寿命预测方法A life prediction method for internal fatigue failure of metal materials

技术领域Technical Field

本发明属于金属材料疲劳失效技术领域,尤其是涉及一种金属材料内部疲劳失效的寿命预测方法。The invention belongs to the technical field of fatigue failure of metal materials, and in particular relates to a life prediction method for internal fatigue failure of metal materials.

背景技术Background Art

随着科学技术的进步,航空航天,汽车,核能等机械结构面对着“轻量化”、“环境适应性”以及“长寿命化”的需求,且它们直接关系到机械机构的服役性能、使用寿命和安全可靠性。对于机械结构而言,其结构材料在服役过程中会受到复杂环境等因素的影响,进而发生高循环的环境-疲劳耦合损伤,大大制约了机械结构高性能-高耐久性-低维修成本的发展需求,迫切需要在结构的材料选用、失效诊断以及寿命预测等方面取得突破性进展。此外,传统机械结构建立在“安全系数为2”或“静设计、动校准”的强度准则,已远不能满足复杂服役环境下机械结构及材料长寿命预测的要求。因此,需要在明确金属结构及材料的疲劳耦合损伤模式、规律及机理的前提下,基于多学科的理论和方法,揭示、分析及构建金属材料环境-疲劳损伤演化方程,形成基于失效机制的高疲劳寿命疲劳耦合损伤评估方法,才能满足机械结构环境-高性能-长寿命设计要求。With the advancement of science and technology, mechanical structures in aerospace, automobiles, nuclear energy, etc. are facing the needs of "lightweight", "environmental adaptability" and "long life", which are directly related to the service performance, service life and safety and reliability of mechanical mechanisms. For mechanical structures, their structural materials will be affected by factors such as complex environment during service, and then high-cycle environmental-fatigue coupling damage will occur, which greatly restricts the development needs of high performance-high durability-low maintenance cost of mechanical structures. It is urgent to make breakthroughs in material selection, failure diagnosis and life prediction of structures. In addition, traditional mechanical structures are based on the strength criteria of "safety factor of 2" or "static design, dynamic calibration", which is far from meeting the requirements of long life prediction of mechanical structures and materials under complex service environments. Therefore, it is necessary to reveal, analyze and construct the environmental-fatigue damage evolution equation of metal materials based on multidisciplinary theories and methods, and form a high fatigue life fatigue coupling damage assessment method based on failure mechanism, so as to meet the requirements of mechanical structure environment-high performance-long life design.

发明内容Summary of the invention

本发明所要解决的技术问题在于针对上述现有技术中的不足,提供一种金属材料内部疲劳失效的寿命预测方法,通过建立基于吉布斯自由能变与内部裂纹萌生时能量演化的关系,随后结合晶体塑性有限元计算循环加载条件下的塑性应变能密度,进而基于能效因子评估对初始吉布斯自由能变方程进行修正,建立细观内部疲劳裂纹萌生寿命预测模型,对金属材料的疲劳寿命进行预估和验证,形成基于失效机制的高疲劳寿命疲劳耦合损伤评估方法,满足了机械结构环境-高性能-长寿命设计要求。The technical problem to be solved by the present invention is to provide a life prediction method for internal fatigue failure of metal materials in response to the deficiencies in the above-mentioned prior art. The method establishes a relationship between the Gibbs free energy change and the energy evolution during internal crack initiation, and then combines the crystal plasticity finite element to calculate the plastic strain energy density under cyclic loading conditions. The initial Gibbs free energy change equation is corrected based on the energy efficiency factor evaluation, and a microscopic internal fatigue crack initiation life prediction model is established. The fatigue life of the metal material is estimated and verified, forming a high fatigue life fatigue coupled damage assessment method based on the failure mechanism, which meets the mechanical structure environment-high performance-long life design requirements.

为解决上述技术问题,本发明采用的技术方案是:一种金属材料内部疲劳失效的寿命预测方法,其特征在于:该方法包括以下步骤:In order to solve the above technical problems, the technical solution adopted by the present invention is: a life prediction method for internal fatigue failure of metal materials, characterized in that the method comprises the following steps:

步骤一、获取加载恒定载荷条件下金属材料的应力-寿命拟合公式:根据金属材料疲劳试验标准,进行周期性载荷加载条件下的恒定载荷疲劳试验,将所得试验数据绘制在坐标系内,通过线性拟合,得到金属材料在恒定载荷加载条件下的应力-寿命曲线和拟合公式lgσa=AlgNf+B;其中,σa为加载的应力幅值,Nf为与加载的应力幅值对应的试验疲劳寿命,A和B为拟合参数;Step 1, obtain the stress-life fitting formula of the metal material under the condition of constant load: according to the fatigue test standard of metal materials, a constant load fatigue test under the condition of periodic load is carried out, the obtained test data is plotted in the coordinate system, and the stress-life curve and fitting formula lgσ a =AlgN f +B of the metal material under the condition of constant load are obtained through linear fitting; wherein, σ a is the loaded stress amplitude, N f is the test fatigue life corresponding to the loaded stress amplitude, and A and B are fitting parameters;

步骤二、获取初始吉布斯自由能变方程:结合吉布斯自由能理论、Mura和Nakasone的理论,得到在对金属材料施加周期性载荷的条件下其内部裂纹萌生过程的能量演化方程为ΔG=-We-Wd+2cvirγs;其中,ΔG为吉布斯自由能变,We为裂纹张开时材料释放的弹性能,Wd为内能存储在金属材料晶格缺陷中的部分外功,cvir为虚拟裂纹长度数值的1/2,γs为裂纹表面能;Step 2, obtaining the initial Gibbs free energy change equation: Combining the Gibbs free energy theory and the theories of Mura and Nakasone, the energy evolution equation of the internal crack initiation process of the metal material under the condition of applying periodic load is obtained as ΔG= -We - Wd + 2cvirγs ; wherein ΔG is the Gibbs free energy change, We is the elastic energy released by the material when the crack opens, Wd is the part of the external work stored in the lattice defects of the metal material by the internal energy, cvir is 1/2 of the virtual crack length value, and γs is the crack surface energy;

步骤三、获取周期性载荷加载条件下的塑性应变能密度:利用有限元软件建立多晶代表体积元模型,采用拉格朗日实体单元对多晶代表体积元模型进行离散,对离散后的多晶代表体积元模型施加周期性载荷,将具有最高塑性应变能密度值的单元作为裂纹萌生的临界单元,则临界单元的塑性应变能密度为

Figure BDA0003982640580000023
Figure BDA0003982640580000021
其中,Δτ为局部剪切应力变化范围,Δγp为对应位置的塑性剪切应变变化范围;Step 3: Obtain the plastic strain energy density under periodic load conditions: Use finite element software to establish a polycrystalline representative volume element model, use Lagrangian solid elements to discretize the polycrystalline representative volume element model, apply periodic loads to the discretized polycrystalline representative volume element model, and use the unit with the highest plastic strain energy density value as the critical unit for crack initiation. The plastic strain energy density of the critical unit is
Figure BDA0003982640580000023
and
Figure BDA0003982640580000021
Among them, Δτ is the variation range of local shear stress, and Δγ p is the variation range of plastic shear strain at the corresponding position;

步骤四、修正初始吉布斯自由能变方程中的裂纹表面能,过程如下:Step 4: Correct the crack surface energy in the initial Gibbs free energy equation. The process is as follows:

步骤401、假设金属材料滑移带中所有位错偶极子均会影响裂纹萌生,则单一滑移带中的位错偶极子数量neq,且

Figure BDA0003982640580000022
其中,b为伯氏矢量,Weq为单一滑移带内部位错偶极子存储的应变能,d为晶粒尺寸,h为滑移带宽度,μ为剪切模量;Step 401: Assuming that all dislocation dipoles in the slip band of the metal material will affect crack initiation, the number of dislocation dipoles in a single slip band is n eq , and
Figure BDA0003982640580000022
Where, b is the Burgers vector, W eq is the strain energy stored in the dislocation dipole inside a single slip band, d is the grain size, h is the slip band width, and μ is the shear modulus;

步骤402、当裂纹萌生结束时,根据Murakami理论,裂纹特征长度为

Figure BDA0003982640580000031
则导致裂纹萌生的最低表面能
Figure BDA0003982640580000032
与Weq之间的关系式为
Figure BDA0003982640580000033
Step 402: When the crack initiation is complete, according to the Murakami theory, the crack characteristic length is
Figure BDA0003982640580000031
The minimum surface energy that leads to crack initiation is
Figure BDA0003982640580000032
The relationship between W eq is
Figure BDA0003982640580000033

步骤403、裂纹长度

Figure BDA0003982640580000034
和伯氏矢量绝对值b与位错数量nc之间的关系为
Figure BDA0003982640580000035
结合步骤401和步骤402,得到位错数量nc的表达式为
Figure BDA0003982640580000036
进而得到裂纹表面能γs的表达式为
Figure BDA0003982640580000037
Step 403: Crack length
Figure BDA0003982640580000034
The relationship between the absolute value of the Burgers vector b and the number of dislocations n c is
Figure BDA0003982640580000035
Combining step 401 and step 402, the expression of the number of dislocations n c is obtained as follows:
Figure BDA0003982640580000036
Then the expression of crack surface energy γs is obtained as
Figure BDA0003982640580000037

步骤五、预估裂纹萌生寿命:根据机械结构中的金属材料,该金属材料的能效因子f保持恒定,结合步骤三和步骤四中的公式可将步骤二中的能量演化方程转化为Step 5: Estimate crack initiation life: According to the metal material in the mechanical structure, the energy efficiency factor f of the metal material remains constant. Combining the formulas in steps 3 and 4, the energy evolution equation in step 2 can be transformed into

Figure BDA0003982640580000038
Figure BDA0003982640580000038

对该公式求偏导可得Taking partial derivative of this formula we get

Figure BDA0003982640580000039
Figure BDA0003982640580000039

当位错偶极子存储的能量与裂纹萌生能量处于平衡状态时,即

Figure BDA00039826405800000310
时,吉布斯自由能变ΔG最大,则When the energy stored in the dislocation dipole is in equilibrium with the crack initiation energy, that is,
Figure BDA00039826405800000310
When , the Gibbs free energy change ΔG is the largest, then

Figure BDA00039826405800000311
Figure BDA00039826405800000311

得到

Figure BDA00039826405800000312
则此时的N为裂纹萌生寿命Ni;get
Figure BDA00039826405800000312
Then N at this time is the crack initiation life Ni ;

另外,Δτ·Δγp为临界单元的塑性应变能密度

Figure BDA00039826405800000314
的两倍,则
Figure BDA00039826405800000313
In addition, Δτ·Δγ p is the plastic strain energy density of the critical element
Figure BDA00039826405800000314
twice of
Figure BDA00039826405800000313

步骤六、验证获取的裂纹萌生寿命精度:以试验疲劳寿命为横坐标,预估裂纹萌生寿命为纵坐标,建立坐标系,将机械结构中的金属材料发生内部失效时的预估裂纹萌生寿命和试验疲劳寿命的比值在坐标系中标出,且机械结构中的金属材料发生内部失效时的预估裂纹萌生寿命和试验疲劳寿命的比值位于3倍线边界内,得出预估的裂纹萌生寿命为该金属材料的内部疲劳失效寿命。Step 6. Verify the accuracy of the obtained crack initiation life: Use the test fatigue life as the horizontal coordinate and the estimated crack initiation life as the vertical coordinate to establish a coordinate system, mark the ratio of the estimated crack initiation life and the test fatigue life when the metal material in the mechanical structure fails internally in the coordinate system, and the ratio of the estimated crack initiation life and the test fatigue life when the metal material in the mechanical structure fails internally is within the 3-fold line boundary, and the estimated crack initiation life is obtained as the internal fatigue failure life of the metal material.

上述的一种金属材料内部疲劳失效的寿命预测方法,其特征在于:步骤二中,裂纹张开时材料释放的弹性能We包括位错本身蕴含的能量和位错偶极子之间相互作用蕴含的能量,则We

Figure BDA0003982640580000041
其中,d为晶粒尺寸,ν为泊松比,k为滑移启动的临界剪切应力,N为循环载荷施加周次,ζ为常数。The above-mentioned life prediction method for internal fatigue failure of a metal material is characterized in that: in step 2, the elastic energy W e released by the material when the crack opens includes the energy contained in the dislocation itself and the energy contained in the interaction between dislocation dipoles, then W e is
Figure BDA0003982640580000041
Where d is the grain size, ν is the Poisson's ratio, k is the critical shear stress for slip initiation, N is the number of cycles of cyclic load application, and ζ is a constant.

上述的一种金属材料内部疲劳失效的寿命预测方法,其特征在于:步骤二中,根据Fine与Bhat的理论可知,Wd为Wd=2cvirNδ;其中,δ为每个循环结束后虚拟裂纹存储的能量。The above-mentioned life prediction method for internal fatigue failure of metal materials is characterized in that: in step 2, according to the theory of Fine and Bhat, W d is W d = 2c vir Nδ; wherein δ is the energy stored in the virtual crack after each cycle ends.

上述的一种金属材料内部疲劳失效的寿命预测方法,其特征在于:根据周期性荷载作用下的恢复力特性曲线,δ为

Figure BDA0003982640580000042
式中,f为能效因子,h为滑移带宽度。The above-mentioned life prediction method for internal fatigue failure of a metal material is characterized in that: according to the characteristic curve of the restoring force under the action of periodic load, δ is
Figure BDA0003982640580000042
Where f is the energy efficiency factor and h is the slip band width.

上述的一种金属材料内部疲劳失效的寿命预测方法,其特征在于:步骤二中,根据位错堆积宽度和虚拟裂纹长度之间的关系,得到虚拟裂纹长度

Figure BDA0003982640580000043
The above-mentioned life prediction method for internal fatigue failure of a metal material is characterized in that: in step 2, the virtual crack length is obtained according to the relationship between the dislocation accumulation width and the virtual crack length.
Figure BDA0003982640580000043

本发明的有益效果是通过建立基于吉布斯自由能变与内部裂纹萌生时能量演化的关系,随后结合晶体塑性有限元计算循环加载条件下的塑性应变能密度,进而基于能效因子评估对初始吉布斯自由能变方程进行修正,建立细观内部疲劳裂纹萌生寿命预测模型,对金属材料的疲劳寿命进行预估和验证,形成基于失效机制的高疲劳寿命疲劳耦合损伤评估方法,满足了机械结构环境-高性能-长寿命设计要求。The beneficial effects of the present invention are as follows: by establishing a relationship between Gibbs free energy change and energy evolution during internal crack initiation, and then combining the crystal plasticity finite element to calculate the plastic strain energy density under cyclic loading conditions, the initial Gibbs free energy change equation is corrected based on the energy efficiency factor evaluation, and a microscopic internal fatigue crack initiation life prediction model is established. The fatigue life of metal materials is estimated and verified, forming a high fatigue life fatigue coupled damage assessment method based on failure mechanism, which meets the mechanical structure environment-high performance-long life design requirements.

下面通过附图和实施例,对本发明的技术方案做进一步的详细描述。The technical solution of the present invention is further described in detail below through the accompanying drawings and embodiments.

附图说明BRIEF DESCRIPTION OF THE DRAWINGS

图1为本发明金属材料SLM-IN718在仿真分析中滑移系为(111)[-110]时最大塑性应变能密度和循环周期数的关系图。FIG. 1 is a graph showing the relationship between the maximum plastic strain energy density and the number of cycles when the slip system is (111)[-110] in the simulation analysis of the metal material SLM-IN718 of the present invention.

图2为本发明金属材料SLM-IN718在仿真分析中滑移系为(111)[0-11]时最大塑性应变能密度和循环周期数的关系图。FIG. 2 is a graph showing the relationship between the maximum plastic strain energy density and the number of cycles when the slip system is (111) [0-11] in the simulation analysis of the metal material SLM-IN718 of the present invention.

图3为本发明金属材料SLM-IN718在仿真分析中预估疲劳寿命和试验疲劳寿命的对比图。FIG3 is a comparison diagram of the estimated fatigue life and the experimental fatigue life of the metal material SLM-IN718 of the present invention in the simulation analysis.

图4为本发明方法的流程框图。FIG4 is a flowchart of the method of the present invention.

具体实施方式DETAILED DESCRIPTION

如图1至图4所示的一种金属材料内部疲劳失效的寿命预测方法,该方法包括以下步骤:A life prediction method for internal fatigue failure of a metal material as shown in FIGS. 1 to 4 comprises the following steps:

步骤一、获取加载恒定载荷条件下金属材料的应力-寿命拟合公式:根据金属材料疲劳试验标准,进行周期性载荷加载条件下的恒定载荷疲劳试验,将所得试验数据绘制在坐标系内,通过线性拟合,得到金属材料在恒定载荷加载条件下的应力-寿命曲线和拟合公式lgσa=AlgNf+B;其中,σa为加载的应力幅值,Nf为与加载的应力幅值对应的试验疲劳寿命,A和B为拟合参数;Step 1, obtain the stress-life fitting formula of the metal material under the condition of constant load: according to the fatigue test standard of metal materials, a constant load fatigue test under the condition of periodic load is carried out, the obtained test data is plotted in the coordinate system, and the stress-life curve and fitting formula lgσ a =AlgN f +B of the metal material under the condition of constant load are obtained through linear fitting; wherein, σ a is the loaded stress amplitude, N f is the test fatigue life corresponding to the loaded stress amplitude, and A and B are fitting parameters;

步骤二、获取初始吉布斯自由能变方程:结合吉布斯自由能理论、Mura和Nakasone的理论,得到在对金属材料施加周期性载荷的条件下其内部裂纹萌生过程的能量演化方程为ΔG=-We-Wd+2cvirγs;其中,ΔG为吉布斯自由能变,We为裂纹张开时材料释放的弹性能,Wd为内能存储在金属材料晶格缺陷中的部分外功,cvir为虚拟裂纹长度数值的1/2,γs为裂纹表面能;Step 2, obtaining the initial Gibbs free energy change equation: Combining the Gibbs free energy theory and the theories of Mura and Nakasone, the energy evolution equation of the internal crack initiation process of the metal material under the condition of applying periodic load is obtained as ΔG= -We - Wd + 2cvirγs ; wherein ΔG is the Gibbs free energy change, We is the elastic energy released by the material when the crack opens, Wd is the part of the external work stored in the lattice defects of the metal material by the internal energy, cvir is 1/2 of the virtual crack length value, and γs is the crack surface energy;

步骤三、获取周期性载荷加载条件下的塑性应变能密度:利用有限元软件建立多晶代表体积元模型,采用拉格朗日实体单元对多晶代表体积元模型进行离散,对离散后的多晶代表体积元模型施加周期性载荷,将具有最高塑性应变能密度值的单元作为裂纹萌生的临界单元,则临界单元的塑性应变能密度为

Figure BDA0003982640580000052
Figure BDA0003982640580000051
其中,Δτ为局部剪切应力变化范围,Δγp为对应位置的塑性剪切应变变化范围;Step 3: Obtain the plastic strain energy density under periodic load conditions: Use finite element software to establish a polycrystalline representative volume element model, use Lagrangian solid elements to discretize the polycrystalline representative volume element model, apply periodic loads to the discretized polycrystalline representative volume element model, and use the unit with the highest plastic strain energy density value as the critical unit for crack initiation. The plastic strain energy density of the critical unit is
Figure BDA0003982640580000052
and
Figure BDA0003982640580000051
Among them, Δτ is the variation range of local shear stress, and Δγ p is the variation range of plastic shear strain at the corresponding position;

步骤四、修正初始吉布斯自由能变方程中的裂纹表面能,过程如下:Step 4: Correct the crack surface energy in the initial Gibbs free energy equation. The process is as follows:

步骤401、假设金属材料滑移带中所有位错偶极子均会影响裂纹萌生,则单一滑移带中的位错偶极子数量neq,且

Figure BDA0003982640580000061
其中,b为伯氏矢量,Weq为单一滑移带内部位错偶极子存储的应变能,d为晶粒尺寸,h为滑移带宽度,μ为剪切模量;Step 401: Assuming that all dislocation dipoles in the slip band of the metal material will affect crack initiation, the number of dislocation dipoles in a single slip band is n eq , and
Figure BDA0003982640580000061
Where, b is the Burgers vector, W eq is the strain energy stored in the dislocation dipole inside a single slip band, d is the grain size, h is the slip band width, and μ is the shear modulus;

步骤402、当裂纹萌生结束时,根据Murakami理论,裂纹特征长度为

Figure BDA0003982640580000062
则导致裂纹萌生的最低表面能
Figure BDA0003982640580000063
与Weq之间的关系式为
Figure BDA0003982640580000064
Step 402: When the crack initiation is complete, according to the Murakami theory, the crack characteristic length is
Figure BDA0003982640580000062
The minimum surface energy that leads to crack initiation is
Figure BDA0003982640580000063
The relationship between W eq is
Figure BDA0003982640580000064

步骤403、裂纹长度

Figure BDA0003982640580000065
和伯氏矢量绝对值b与位错数量nc之间的关系为
Figure BDA0003982640580000066
结合步骤401和步骤402,得到位错数量nc的表达式为
Figure BDA0003982640580000067
进而得到裂纹表面能γs的表达式为
Figure BDA0003982640580000068
Step 403: Crack length
Figure BDA0003982640580000065
The relationship between the absolute value of the Burgers vector b and the number of dislocations n c is
Figure BDA0003982640580000066
Combining step 401 and step 402, the expression of the number of dislocations n c is obtained as follows:
Figure BDA0003982640580000067
Then the expression of crack surface energy γs is obtained as
Figure BDA0003982640580000068

步骤五、预估裂纹萌生寿命:根据机械结构中的金属材料,该金属材料的能效因子f保持恒定,结合步骤三和步骤四中的公式可将步骤二中的能量演化方程转化为Step 5: Estimate crack initiation life: According to the metal material in the mechanical structure, the energy efficiency factor f of the metal material remains constant. Combining the formulas in steps 3 and 4, the energy evolution equation in step 2 can be transformed into

Figure BDA0003982640580000069
Figure BDA0003982640580000069

对该公式求偏导可得Taking partial derivative of this formula we get

Figure BDA00039826405800000610
Figure BDA00039826405800000610

当位错偶极子存储的能量与裂纹萌生能量处于平衡状态时,即

Figure BDA00039826405800000611
时,吉布斯自由能变ΔG最大,则When the energy stored in the dislocation dipole is in equilibrium with the crack initiation energy, that is,
Figure BDA00039826405800000611
When , the Gibbs free energy change ΔG is the largest, then

Figure BDA00039826405800000612
Figure BDA00039826405800000612

得到

Figure BDA0003982640580000071
则此时的N为裂纹萌生寿命Ni;get
Figure BDA0003982640580000071
Then N at this time is the crack initiation life Ni ;

另外,Δτ·Δγp为临界单元的塑性应变能密度

Figure BDA0003982640580000073
的两倍,则
Figure BDA0003982640580000072
In addition, Δτ·Δγ p is the plastic strain energy density of the critical element
Figure BDA0003982640580000073
twice of
Figure BDA0003982640580000072

步骤六、验证获取的裂纹萌生寿命精度:以试验疲劳寿命为横坐标,预估裂纹萌生寿命为纵坐标,建立坐标系,将机械结构中的金属材料发生内部失效时的预估裂纹萌生寿命和试验疲劳寿命的比值在坐标系中标出,且机械结构中的金属材料发生内部失效时的预估裂纹萌生寿命和试验疲劳寿命的比值位于3倍线边界内,得出预估的裂纹萌生寿命为该金属材料的内部疲劳失效寿命。Step 6. Verify the accuracy of the obtained crack initiation life: Use the test fatigue life as the horizontal coordinate and the estimated crack initiation life as the vertical coordinate to establish a coordinate system, mark the ratio of the estimated crack initiation life and the test fatigue life when the metal material in the mechanical structure fails internally in the coordinate system, and the ratio of the estimated crack initiation life and the test fatigue life when the metal material in the mechanical structure fails internally is within the 3-fold line boundary, and the estimated crack initiation life is obtained as the internal fatigue failure life of the metal material.

本发明通过建立基于吉布斯自由能变与内部裂纹萌生时能量演化的关系,随后结合晶体塑性有限元计算循环加载条件下的塑性应变能密度,进而基于能效因子评估对初始吉布斯自由能变方程进行修正,建立细观内部疲劳裂纹萌生寿命预测模型,对金属材料的疲劳寿命进行预估和验证,形成基于失效机制的高疲劳寿命疲劳耦合损伤评估方法,满足了机械结构环境-高性能-长寿命设计要求。The present invention establishes a relationship between Gibbs free energy change and the energy evolution during internal crack initiation, and then combines the crystal plasticity finite element to calculate the plastic strain energy density under cyclic loading conditions, and then corrects the initial Gibbs free energy change equation based on energy efficiency factor evaluation, establishes a micro-internal fatigue crack initiation life prediction model, estimates and verifies the fatigue life of metal materials, and forms a high fatigue life fatigue coupled damage assessment method based on failure mechanism, which meets the mechanical structure environment-high performance-long life design requirements.

步骤一中的应力-寿命曲线中,是以试验疲劳寿命为横坐标,应力幅值为纵坐标建立坐标系。In the stress-life curve in step 1, the coordinate system is established with the test fatigue life as the horizontal axis and the stress amplitude as the vertical axis.

实际使用时,金属材料在周期性载荷作用下发生疲劳断裂的过程可以视作材料形成新表面的过程,且疲劳载荷涉及反复的加载与卸载过程;而Mura和Nakasone认为在卸载过程中由反向滑移形成的位错偶极子会随着载荷地持续施加而不断累积,因此可得到步骤二中的能量演化方程。In actual use, the process of fatigue fracture of metal materials under periodic loads can be regarded as the process of forming a new surface of the material, and the fatigue load involves repeated loading and unloading processes; Mura and Nakasone believe that the dislocation dipoles formed by reverse slip during the unloading process will continue to accumulate as the load continues to be applied, so the energy evolution equation in step two can be obtained.

步骤三中,基于所选取的本构方程拟合材料参数,当应力-应变关系计算值与实测值一致性较好时表明该组材料参数可以用于后续塑性应变能密度计算。通过修改载荷谱,对模型施加循环载荷,在循环载荷作用下晶粒的塑性应变能密度是晶体塑性有限元计算结果中十分重要的参数,该参数已被用于预测裂纹萌生寿命。单一晶粒具有特定的晶粒取向,因此在仿真计算过程中,可将具有最高塑性应变能密度值的单元视为裂纹萌生的临界位置,且最大塑性应变能密度值会在一定循环周次后趋于稳定。当最大塑性应变能密度值稳定后,模型在不同循环载荷周次内求得的计算结果相近,因此可将该时刻的计算结果用于后续分析与研究,因此可以从计算结果中提取相应的Δτ与Δγp以计算塑性应变能密度。In step three, the material parameters are fitted based on the selected constitutive equation. When the calculated value of the stress-strain relationship is consistent with the measured value, it indicates that this set of material parameters can be used for subsequent plastic strain energy density calculation. By modifying the load spectrum and applying cyclic loads to the model, the plastic strain energy density of the grain under cyclic loads is a very important parameter in the crystal plastic finite element calculation results. This parameter has been used to predict the crack initiation life. A single grain has a specific grain orientation. Therefore, in the simulation calculation process, the unit with the highest plastic strain energy density value can be regarded as the critical position of crack initiation, and the maximum plastic strain energy density value will tend to stabilize after a certain number of cycles. When the maximum plastic strain energy density value is stable, the calculation results obtained by the model in different cyclic load cycles are similar, so the calculation results at this moment can be used for subsequent analysis and research. Therefore, the corresponding Δτ and Δγ p can be extracted from the calculation results to calculate the plastic strain energy density.

如图1和图2所示,为前25个周期内某一位置处不同滑移系最大塑性应变能密度数值随着循环周次的变化关系,可以看出,如图1所示,滑移面(111)滑移方向[-110]的滑移系上最大塑性应变能密度随着循环周次增加而升高,而如图2所示,滑移面(111)滑移方向[0,-1,1]的滑移系上最大塑性应变能密度随着循环周次的升高而降低,二者均在当载荷数大于15周次时趋于稳定。在进行金属材料SLM-IN718的超高周疲劳特性仿真分析时,为了降低计算成本,因此以最大塑性应变能密度稳定时的应力、应变状态作为参考,而不用计算整个超高周疲劳循环周次,故在后续分析中均以第20周的计算结果为依据。As shown in Figures 1 and 2, the maximum plastic strain energy density values of different slip systems at a certain position in the first 25 cycles vary with the number of cycles. It can be seen that, as shown in Figure 1, the maximum plastic strain energy density on the slip system with the slip direction [-110] of the slip plane (111) increases with the increase of the number of cycles, while as shown in Figure 2, the maximum plastic strain energy density on the slip system with the slip direction [0, -1, 1] of the slip plane (111) decreases with the increase of the number of cycles. Both tend to be stable when the load number is greater than 15 cycles. In the simulation analysis of the ultra-high cycle fatigue characteristics of the metal material SLM-IN718, in order to reduce the calculation cost, the stress and strain state when the maximum plastic strain energy density is stable is used as a reference, instead of calculating the entire ultra-high cycle fatigue cycle. Therefore, the calculation results of the 20th week are used as the basis in the subsequent analysis.

步骤四中,滑移带为由一组平行的滑移线构成的带,当晶体在切应力作用下产生滑移时,在晶体表面形成显微台阶,在显微镜下观察时是一些细线,称滑移线,滑移线常成组出现,形成滑移带。滑移带是晶体发生塑性变形的重要特征。In step 4, the slip band is a band composed of a group of parallel slip lines. When the crystal slips under the action of shear stress, microscopic steps are formed on the surface of the crystal. When observed under a microscope, they are some thin lines, called slip lines. Slip lines often appear in groups to form slip bands. Slip bands are an important feature of plastic deformation of crystals.

步骤五中,从裂纹萌生初始时刻开始,吉布斯自由能变ΔG为正表示存在判定裂纹是否萌生的能量限界。当位错偶极子蕴含能量与裂纹萌生能量处于平衡状态时,此时自由能最大。而后随着循环载荷继续施加,裂纹自由能逐渐减小,裂纹完全萌生时刻位错偶极子结构失稳。因此以吉布斯自由能最大时刻作为裂纹萌生完成时刻。简而言之,裂纹萌生的G随着裂纹的增长而增长,且当时达到临界值。步骤五中,根据机械结构中的金属材料,得到该金属材料的能效因子

Figure BDA0003982640580000081
其中,σmax为施加载荷中的最大载荷值,E为弹性模量;In step five, starting from the initial moment of crack initiation, the Gibbs free energy change ΔG becomes positive, indicating that there is an energy limit for determining whether the crack has initiated. When the energy contained in the dislocation dipole and the crack initiation energy are in equilibrium, the free energy is maximum. Then, as the cyclic load continues to be applied, the crack free energy gradually decreases, and the dislocation dipole structure becomes unstable when the crack is fully initiated. Therefore, the moment of maximum Gibbs free energy is taken as the moment when crack initiation is completed. In short, the G of crack initiation increases with the growth of the crack, and reaches a critical value at that time. In step five, based on the metal material in the mechanical structure, the energy efficiency factor of the metal material is obtained.
Figure BDA0003982640580000081
Wherein, σ max is the maximum load value in the applied load, and E is the elastic modulus;

需要说明的是,如图3所示,在进行金属材料SLM-IN718预估疲劳寿命和试验疲劳寿命的对比图中R为应力比,即最小应力值和最大应力值的比值;3倍线为疲劳寿命试验中校验精度的标准,坐标系是以试验疲劳寿命为横坐标x,预估裂纹萌生寿命为纵坐标y,则图中的虚线为y=x时的界限,两条实线分别为y=3x时的线条、

Figure BDA0003982640580000091
时的线条。It should be noted that, as shown in FIG3 , in the comparison diagram of the estimated fatigue life and the experimental fatigue life of metal material SLM-IN718, R is the stress ratio, that is, the ratio of the minimum stress value to the maximum stress value; the 3-fold line is the standard for verifying the accuracy in the fatigue life test, and the coordinate system is based on the experimental fatigue life as the horizontal coordinate x and the estimated crack initiation life as the vertical coordinate y. The dotted line in the figure is the limit when y=x, and the two solid lines are the lines when y=3x,
Figure BDA0003982640580000091
The lines of time.

本实施例中,步骤二中,裂纹张开时材料释放的弹性能We包括位错本身蕴含的能量和位错偶极子之间相互作用蕴含的能量,则We

Figure BDA0003982640580000092
其中,d为晶粒尺寸,ν为泊松比,k为滑移启动的临界剪切应力,N为循环载荷施加周次,ζ为常数。In this embodiment, in step 2, the elastic energy We released by the material when the crack opens includes the energy contained in the dislocation itself and the energy contained in the interaction between dislocation dipoles, so We is
Figure BDA0003982640580000092
Where d is the grain size, ν is the Poisson's ratio, k is the critical shear stress for slip initiation, N is the number of cycles of cyclic load application, and ζ is a constant.

本实施例中,步骤二中,根据Fine与Bhat的理论可知,Wd为Wd=2cvirNδ;其中,δ为每个循环结束后虚拟裂纹存储的能量。In this embodiment, in step 2, according to the theory of Fine and Bhat, W d is W d = 2c vir Nδ, where δ is the energy stored in the virtual crack after each cycle.

本实施例中,根据周期性荷载作用下的恢复力特性曲线,δ为

Figure BDA0003982640580000093
式中,f为能效因子,h为滑移带宽度。In this embodiment, according to the characteristic curve of the restoring force under periodic load, δ is
Figure BDA0003982640580000093
Where f is the energy efficiency factor and h is the slip band width.

本实施例中,步骤二中,根据位错堆积宽度和虚拟裂纹长度之间的关系,得到虚拟裂纹长度

Figure BDA0003982640580000094
In this embodiment, in step 2, the virtual crack length is obtained based on the relationship between the dislocation accumulation width and the virtual crack length.
Figure BDA0003982640580000094

以上所述,仅是本发明的较佳实施例,并非对本发明作任何限制,凡是根据本发明技术实质对以上实施例所作的任何简单修改、变更以及等效结构变化,均仍属于本发明技术方案的保护范围内。The above description is only a preferred embodiment of the present invention and does not limit the present invention in any way. Any simple modification, change and equivalent structural change made to the above embodiment based on the technical essence of the present invention still falls within the protection scope of the technical solution of the present invention.

Claims (5)

1. A method for predicting the service life of internal fatigue failure of a metal material is characterized by comprising the following steps:
step one, obtaining a stress-life fitting formula of a metal material under a constant load loading condition: according to the fatigue test standard of the metal material, performing a constant load fatigue test under the condition of periodic load loading, drawing the obtained test data in a coordinate system, and obtaining a stress-life curve and a fitting formula lg sigma of the metal material under the condition of constant load loading through linear fitting a =AlgN f + B; wherein σ a Magnitude of stress for load, N f The test fatigue life corresponding to the loaded stress amplitude is shown, and A and B are fitting parameters;
step two, obtaining an initial Gibbs free energy variable equation: combining Gibbs free energy theory and Mura and Nakasone theory to obtain an energy evolution equation of delta G = -W in the internal crack initiation process under the condition of applying periodic load to the metal material e -W d +2c vir γ s (ii) a Wherein Δ G is Gibbs free energy change, W e The elastic energy released by the material when the crack opens, W d A part of external work stored in lattice defects of the metal material as internal energy, c vir Is 1/2, gamma of the virtual crack length value s Is the crack surface energy;
step three, obtaining the plastic strain energy density under the condition of periodic load loading: establishing a polycrystal representative volume element model by using finite element software, dispersing the polycrystal representative volume element model by adopting Lagrange entity units, applying periodic load to the dispersed polycrystal representative volume element model, taking the unit with the highest plastic strain energy density value as a critical unit for crack initiation, and then setting the plastic strain energy density of the critical unit as
Figure FDA0003982640570000011
And is
Figure FDA0003982640570000012
Wherein, delta tau is the variation range of local shear stress, delta gamma p The plastic shear strain variation range of the corresponding position;
step four, correcting the surface energy of the crack in the initial Gibbs free energy variable equation, wherein the process is as follows:
step 401, assuming that all dislocation dipoles in the slip band of the metal material can affect crack initiation, the number n of dislocation dipoles in a single slip band eq And is and
Figure FDA0003982640570000013
wherein b is a Boehringer vector, W eq Strain energy stored by dislocation dipoles inside a single slip band, d is the size of a crystal grain, h is the width of the slip band, and mu is shear modulus;
step 402, when the crack initiation is finished, according to the Murakami theory, the crack characteristic length is
Figure FDA0003982640570000021
The lowest surface energy leading to crack initiation
Figure FDA0003982640570000022
And W eq The relation between is
Figure FDA0003982640570000023
Step 403, crack length
Figure FDA0003982640570000024
Absolute value of the sum-Boehringer vector b and number of dislocations n c The relationship between is
Figure FDA0003982640570000025
Combining the step 401 and the step 402 to obtain the dislocation number n c Is expressed as
Figure FDA0003982640570000026
Thereby obtaining the surface energy gamma of the cracks s Is expressed as
Figure FDA0003982640570000027
And fifthly, estimating the crack initiation life: according to the metal material in the mechanical structure, the energy efficiency factor f of the metal material is kept constant, and the energy evolution equation in the step two can be converted into the energy evolution equation in the step three and the energy evolution equation in the step four by combining the formulas in the step three and the step four
Figure FDA0003982640570000028
The formula is calculated to obtain the deviation
Figure FDA0003982640570000029
When the energy stored by the dislocation dipole is in equilibrium with the crack initiation energy, i.e.
Figure FDA00039826405700000210
When the change of Gibbs free energy is maximum, the
Figure FDA00039826405700000211
To obtain
Figure FDA00039826405700000212
N at this time is the crack initiation life N i
In addition, Δ τ Δ γ p Is the plastic strain energy density of the critical unit
Figure FDA00039826405700000213
Twice of, then
Figure FDA00039826405700000214
Step six, verifying the obtained crack initiation life precision: the method comprises the steps of taking the test fatigue life as an abscissa and the predicted crack initiation life as an ordinate, establishing a coordinate system, marking the ratio of the predicted crack initiation life to the test fatigue life when the metal material in the mechanical structure is subjected to internal failure in the coordinate system, and locating the ratio of the predicted crack initiation life to the test fatigue life when the metal material in the mechanical structure is subjected to internal failure in a 3-fold line boundary to obtain the predicted crack initiation life as the internal fatigue failure life of the metal material.
2. The method for predicting the service life of the internal fatigue failure of the metal material according to claim 1, wherein: in the second step, the elastic energy W released by the material when the crack opens e Including the energy contained in the dislocations themselves and the energy contained in the interactions between the dislocation dipoles, W e Is composed of
Figure FDA0003982640570000031
Wherein d is the crystal grain size, v is the Poisson ratio, k is the critical shear stress of slip start, N is the cycle of applying cyclic load, and zeta is a constant.
3. The method for predicting the service life of the internal fatigue failure of the metal material as recited in claim 1, wherein: in the second step, W can be known according to the theory of Fine and Bhat d Is W d =2c vir N delta; where δ is the energy stored by the virtual crack after the end of each cycle.
4. The method for predicting the life of the internal fatigue failure of the metal material according to claim 3, wherein: according to the characteristic curve of the restoring force under the action of the periodic load, delta is
Figure FDA0003982640570000032
In the formula, f is an energy efficiency factor, and h is the width of the slip band.
5. The method for predicting the service life of the internal fatigue failure of the metal material as recited in claim 1, wherein: in the second step, the virtual crack length is obtained according to the relationship between the dislocation pile-up width and the virtual crack length
Figure FDA0003982640570000033
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CN116738804A (en) * 2023-08-16 2023-09-12 湖南大学 A power module life prediction method based on failure physics

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* Cited by examiner, † Cited by third party
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CN116738804A (en) * 2023-08-16 2023-09-12 湖南大学 A power module life prediction method based on failure physics
CN116738804B (en) * 2023-08-16 2023-11-03 湖南大学 Power module life prediction method based on failure physics

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