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CN111610109A - A creep strain calculation method of a material under small punch test and its application - Google Patents

A creep strain calculation method of a material under small punch test and its application Download PDF

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CN111610109A
CN111610109A CN201910138791.7A CN201910138791A CN111610109A CN 111610109 A CN111610109 A CN 111610109A CN 201910138791 A CN201910138791 A CN 201910138791A CN 111610109 A CN111610109 A CN 111610109A
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赵雷
宋恺
徐连勇
韩永典
荆洪阳
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Abstract

本发明基于小冲杆技术建立了一种材料在小冲杆试验下的蠕变应变计算方法及其应用,所述计算方法包括:理论变形模型的建立与相关关系的获得、建立等效蠕变应变与试样中心挠曲变形之间的关系及公式简化、材料蠕变应变性能的预测。本发明解决传统单轴蠕变试验在小冲孔蠕变试验中的局限性,获得小冲孔蠕变试验中无法直接获得的重要材料参数,对材料蠕变应变的计算精度较高。

Figure 201910138791

The invention establishes a creep strain calculation method and application of materials under the small punch test based on the small punch technology. The relationship between strain and flexural deformation at the center of the sample and the simplification of the formula, the prediction of the creep strain performance of the material. The invention solves the limitation of the traditional uniaxial creep test in the small punching creep test, obtains important material parameters that cannot be directly obtained in the small punching creep test, and has high calculation accuracy for the material creep strain.

Figure 201910138791

Description

一种材料在小冲杆试验下的蠕变应变计算方法及其应用A creep strain calculation method of a material under small punch test and its application

技术领域technical field

本发明涉及高温服役材料性能评估技术领域,特别是涉及一种材料在小冲杆试验下的蠕变应变计算方法及其应用。The invention relates to the technical field of material performance evaluation in high temperature service, in particular to a method for calculating creep strain of a material under a small punch test and its application.

背景技术Background technique

在核电、石油化工等领域中,高温高压等恶劣服役条件会使材料随着服役时间的增加而产生劣化和损伤,并逐渐降低材料的力学性能,最终导致设备、仪器的突发性破坏,造成不可挽回的重大损失,甚至人员伤亡。因此,如何准确评估服役材料在蠕变过程的剩余寿命,具有深远的现实意义。In the fields of nuclear power, petrochemical and other fields, harsh service conditions such as high temperature and high pressure will cause deterioration and damage to materials with the increase of service time, and gradually reduce the mechanical properties of materials, eventually leading to sudden damage to equipment and instruments, resulting in Irreversible heavy losses and even casualties. Therefore, how to accurately evaluate the remaining life of service materials during the creep process has far-reaching practical significance.

目前而言,常用的方法是利用小冲孔蠕变试验在服役部件上获取一定量材料,制备试样后进行蠕变试验。研究人员将小冲孔蠕变试验条件下获得的中心挠曲变形-时间曲线与单轴蠕变试验曲线进行对比,利用两者之间的相似性进行性能分析,进而预测服役材料的剩余寿命。大多数的研究是将小冲孔试验中的载荷利用线性转化关系计算出单轴蠕变试验下的等效应力后,利用单轴应力下得到的蠕变应变或断裂时间等参数,进行进一步蠕变性能的分析与研究。然而,小冲孔蠕变试验与单轴蠕变试验存在一定的差异,如小冲孔试验中试样处于多轴应力状态,且试样上的载荷会受到试样变形的影响。因此,直接将小冲孔蠕变试验的载荷转化为单轴试验的等效应力具有一定的局限性。而小冲孔蠕变试验过程只能获得试样在蠕变过程中的中心挠曲变形,无法直接试样变形过程中的等效蠕变应变。At present, the commonly used method is to obtain a certain amount of material on the service part by using the small punching creep test, and then perform the creep test after preparing the sample. The researchers compared the central flexural deformation-time curve obtained under the small punching creep test condition with the uniaxial creep test curve, and used the similarity between the two to conduct performance analysis to predict the remaining life of the service material. Most of the research is to use the load in the small punching test to calculate the equivalent stress under the uniaxial creep test by using the linear transformation relationship, and then use the parameters such as creep strain or rupture time obtained under the uniaxial stress to carry out further creep. Analysis and research of variable performance. However, there are certain differences between the small punching creep test and the uniaxial creep test. For example, in the small punching test, the sample is in a state of multiaxial stress, and the load on the sample is affected by the deformation of the sample. Therefore, the direct conversion of the load of the small punching creep test into the equivalent stress of the uniaxial test has certain limitations. The small punching creep test process can only obtain the center deflection deformation of the sample during the creep process, and cannot directly obtain the equivalent creep strain during the sample deformation process.

由此可见,现在迫切需要研究一种在小冲孔蠕变试验条件下获得蠕变应变的计算方法,以满足材料蠕变性能的精确分析及寿命预测需求。It can be seen that there is an urgent need to study a calculation method for obtaining creep strain under the condition of small punching creep test, so as to meet the requirements of accurate analysis of material creep performance and life prediction.

发明内容SUMMARY OF THE INVENTION

本发明的目的在于提供一种材料在小冲孔蠕变试验下的蠕变应变计算方法,该方法可有效地解决现有小冲孔蠕变试验下无法获的材料蠕变应变等问题,为应用在高温高压条件下重要部件的蠕变性能评估提供一种新的方法。The purpose of the present invention is to provide a method for calculating the creep strain of materials under the small punching creep test, which can effectively solve the problems of the material creep strain that cannot be obtained under the existing small punching creep test, and is It provides a new method for evaluating the creep performance of important components under high temperature and high pressure conditions.

本发明的另一方面,是提供一种所述蠕变应变计算方法在评估服役材料在蠕变过程的剩余寿命中的应用,可简化评估步骤,评估准确率高。Another aspect of the present invention is to provide an application of the creep strain calculation method in evaluating the remaining life of a service material in a creep process, which can simplify the evaluation steps and have a high evaluation accuracy.

为实现本发明的目的所采用的技术方案是:The technical scheme adopted for realizing the purpose of the present invention is:

一种材料在小冲孔蠕变试验下的蠕变应变计算方法,包括以下步骤:A method for calculating creep strain of a material under a small punching creep test, comprising the following steps:

步骤1,分析不同材料在小冲杆蠕变过程中的变形规律,将小冲杆试样分为三个变形区域,即球形区域a,不等壁厚锥体区域b和等壁厚区域c,建立基于试验条件的理论变形模型关系式(1)-(3)。Step 1, analyze the deformation law of different materials in the small punch creep process, and divide the small punch sample into three deformation areas, namely spherical area a, unequal wall thickness cone area b and equal wall thickness area c , and establish the theoretical deformation model relations (1)-(3) based on the experimental conditions.

Figure BDA0001977865200000021
Figure BDA0001977865200000021

Figure BDA0001977865200000022
Figure BDA0001977865200000022

VC=π[R2-(R-A)2]h0 (3)V C =π[R 2 -(RA) 2 ]h 0 (3)

式(1)、(2)和(3)中:VA为球形区域a的体积,mm3,VB为不等壁厚锥体区域b的体积,mm3,VC为等壁厚区域c的体积,mm3,r为冲球半径,mm;hmin为最小试样厚度,mm;α为试样中心线与试样下表面夹角,°;h0为初始试样厚度,mm;A为等壁厚区域c的宽度,mm;R为试样半径,mm;In formulas (1), (2) and (3): VA is the volume of spherical area a , mm 3 , VB is the volume of cone area b with unequal wall thickness, mm 3 , VC is the area of equal wall thickness The volume of c, mm 3 , r is the radius of the punching ball, mm; h min is the minimum sample thickness, mm; α is the angle between the center line of the sample and the lower surface of the sample, °; h0 is the initial sample thickness, mm; A is the width of the equal wall thickness area c, mm; R is the radius of the sample, mm;

步骤2,根据试样变形过程中体积不变原理,利用式(4)建立小冲孔蠕变试验中心挠曲变形-试样中心与变形区域夹角之间,试样厚度-中心挠曲变形之间的关系式(5)和(6)。利用式(5)和(6)和试验数据,建立试样厚度-试样中心挠曲变形的对应关系,即hmin=f(L)。Step 2: According to the principle of constant volume during the deformation of the sample, formula (4) is used to establish the center deflection deformation of the small punching creep test - the angle between the center of the sample and the deformation area, the thickness of the sample - the center deflection deformation The relationship between (5) and (6). Using equations (5) and (6) and the test data, the corresponding relationship between the thickness of the sample and the deflection of the center of the sample is established, that is, h min =f(L).

VA+VB+VC=πR2h0 (4)V A +V B +V C =πR 2 h 0 (4)

Figure BDA0001977865200000023
Figure BDA0001977865200000023

Figure BDA0001977865200000024
Figure BDA0001977865200000024

式中:L为试验过程中采集的试样中心挠曲变形,mm;In the formula: L is the deflection deformation of the sample center collected during the test, mm;

步骤3,利用Chakrabarty提出的小冲孔蠕变试验中等效蠕变应变与试样厚度之间的关系式(7):Step 3, use the relationship between the equivalent creep strain and the thickness of the sample in the small punching creep test proposed by Chakrabarty (7):

ε=ln(h0/hmin) (7)ε=ln(h 0 /h min ) (7)

式中:ε为小冲杆试样等效蠕变应变,无量纲参数。where ε is the equivalent creep strain of the small punch sample, a dimensionless parameter.

由于hmin=f(L),建立基于理想变形模型的等效蠕变应变与试样中心挠曲变形之间的关系式(8);Since h min = f(L), the relationship between the equivalent creep strain based on the ideal deformation model and the deflection deformation at the center of the sample is established (8);

ε=ln(h0/f(L)) (8)ε=ln(h 0 /f(L)) (8)

步骤4,将步骤2和3中得到的关系式(5)、(6)和(8)耦合进小冲孔蠕变试验中采集的中心挠曲变形数据中,得到小冲孔蠕变试验蠕变应变与试样中心挠曲变形之间的对应关系。为了便于工程实际应用,采用式(9)进行非线性拟合,得到小冲孔蠕变试验中蠕变应变与中心挠曲变形关系式中的重要物理参数a、b、c、d,建立小冲孔蠕变试验蠕变应变与中心挠曲变形关系表达式;In step 4, the relational expressions (5), (6) and (8) obtained in steps 2 and 3 are coupled into the central flexural deformation data collected in the small punching creep test to obtain the small punching creep test creep. Correspondence between variable strain and flexural deformation at the center of the specimen. In order to facilitate the practical application of engineering, the nonlinear fitting is carried out by formula (9), and the important physical parameters a, b, c and d in the relationship between the creep strain and the central flexural deformation in the small punching creep test are obtained. The expression of the relationship between the creep strain and the center deflection deformation of the punching creep test;

ε=a(L/h0)4+b(L/h0)3+c(L/h0)2+d(L/h0) (9)ε=a(L/h 0 ) 4 +b(L/h 0 ) 3 +c(L/h 0 ) 2 +d(L/h 0 ) (9)

步骤5,将式(9)耦合入小冲孔蠕变试验直接获得的中心挠曲变形-时间曲线数据中,最终建立小冲孔蠕变试验蠕变应变与试验时间的关系图。In step 5, formula (9) is coupled into the central flexural deformation-time curve data directly obtained by the small punching creep test, and finally the relationship between the creep strain and the test time of the small punching creep test is established.

本发明的另一方面,还包括所述材料在试验条件下的蠕变应变计算方法在评估服役材料在蠕变过程的剩余寿命中的应用。Another aspect of the present invention further includes the application of the method for calculating the creep strain of the material under test conditions in evaluating the remaining life of the service material in the creep process.

在上述技术方案中,所述服役材料为Sanicro25奥氏体不锈钢。In the above technical solution, the service material is Sanicro25 austenitic stainless steel.

在上述技术方案中,所述服役材料的服役温度为500-100摄氏度。In the above technical solution, the service temperature of the service material is 500-100 degrees Celsius.

与现有技术相比,本发明的有益效果是:Compared with the prior art, the beneficial effects of the present invention are:

1.本发明基于小冲杆技术建立了一种材料在试验条件下的蠕变应变计算方法,解决传统单轴蠕变试验在小冲孔蠕变试验中的局限性,获得小冲孔蠕变试验中无法直接获得的重要材料参数,对材料蠕变应变的计算精度较高。1. The present invention establishes a creep strain calculation method for materials under test conditions based on the small punch technology, solves the limitations of the traditional uniaxial creep test in the small punch creep test, and obtains the small punch creep. Important material parameters that cannot be directly obtained in the test have high calculation accuracy for material creep strain.

2.计算过程中理论变形模型的建立以试验为基础,准确度高;2. The establishment of the theoretical deformation model in the calculation process is based on experiments, with high accuracy;

3.获得的经验公式形式简单,便于普及与应用;3. The obtained empirical formula has a simple form, which is convenient for popularization and application;

4.计算效率高,对材料蠕变应变的计算精度较高;4. The calculation efficiency is high, and the calculation accuracy of the material creep strain is high;

5.可替代单轴蠕变试验,所需要的数据可由小冲孔蠕变试验获得,降低成本。5. It can replace the uniaxial creep test, and the required data can be obtained by the small punching creep test to reduce the cost.

附图说明Description of drawings

图1是本发明中小冲孔蠕变试验下的蠕变应变计算方法研究路线示意图。Fig. 1 is a schematic diagram of the research route of the creep strain calculation method under the small and medium punching creep test of the present invention.

图2是小冲杆蠕变试验曲线。Figure 2 is the small punch creep test curve.

图3是小冲杆试样剖面显微金相图分析图。Figure 3 is a microscopic metallographic analysis diagram of the cross-section of the small punch sample.

图4是试验过程的小冲杆试样变形示意图。Figure 4 is a schematic diagram of the deformation of the small punch sample during the test.

图5是小冲杆蠕变试验试样厚度-中心挠曲变形曲线图。Figure 5 is a graph of the thickness-center deflection curve of the small punch creep test specimen.

图6是典型的小冲杆蠕变试验中蠕变应变-(L/h0)曲线图。Figure 6 is a graph of creep strain-(L/h 0 ) in a typical small punch creep test.

图7是本发明提出的蠕变应变计算方法与有限元计算结果对比曲线图。FIG. 7 is a graph showing the comparison between the creep strain calculation method proposed by the present invention and the finite element calculation results.

具体实施方式Detailed ways

下面结合具体实施例和附图,进一步阐述本发明。The present invention will be further described below with reference to specific embodiments and accompanying drawings.

请参阅图1所示,本发明提供一种材料在小冲孔蠕变试验下的蠕变应变计算方法,包括:理论变形模型的建立与相关关系的获得、建立等效蠕变应变与试样中心挠曲变形之间的关系及公式简化、材料蠕变应变性能的预测。以Sanicro25奥氏体不锈钢为例,不同载荷条件下小冲孔蠕变试验直接获得的中心挠曲变形-时间曲线如图2所示,为了得到试样在试验过程中的蠕变应变,具体步骤如下:Referring to Fig. 1, the present invention provides a method for calculating creep strain of materials under a small punching creep test, including: establishing a theoretical deformation model and obtaining a correlation, establishing an equivalent creep strain and a sample The relationship between the central deflection and the simplification of the formula, the prediction of the creep strain performance of the material. Taking Sanicro25 austenitic stainless steel as an example, the central flexural deformation-time curve obtained directly from the small punching creep test under different load conditions is shown in Figure 2. In order to obtain the creep strain of the sample during the test, the specific steps as follows:

第一步,利用小冲杆试样剖面显微金相图分析试验中试样变形规律,如图3所示。试样在试验过程中的变形主要可以分为三部分,(1)与冲压球接触的球形区域A,厚度均匀,为最小值hmin;(2)不等厚度锥体区域B,厚度从球形区域的hmin线性递增至试样初始厚度h0;(3)等厚度锥体区域C,厚度均匀,为初始试样厚度h0。根据试样的变形规律及体积不变原则,建立如图4所示的小冲孔蠕变试验理论变形模型。本实例中下模孔径R为0.2mm,c区域宽度A为0.02mm,试样初始厚度h0为0.5mm,冲球半径r为1.25mm。根据式(5)可以建立试样厚度-夹角α之间的关系式(10):The first step is to analyze the deformation law of the sample in the test by using the microscopic metallographic diagram of the cross-section of the small punch sample, as shown in Figure 3. The deformation of the sample during the test can be mainly divided into three parts, (1) the spherical area A in contact with the punching ball, the thickness is uniform, and is the minimum value h min ; (2) the unequal thickness cone area B, the thickness is from the spherical area. The h min of the region increases linearly to the initial thickness h 0 of the sample; (3) the equal thickness cone region C, with uniform thickness, is the initial sample thickness h 0 . According to the deformation law of the sample and the principle of constant volume, the theoretical deformation model of the small punching creep test as shown in Figure 4 is established. In this example, the aperture R of the lower die is 0.2 mm, the width A of the c region is 0.02 mm, the initial thickness h 0 of the sample is 0.5 mm, and the radius r of the punching ball is 1.25 mm. According to the formula (5), the relationship between the thickness of the sample and the angle α can be established (10):

Figure BDA0001977865200000041
Figure BDA0001977865200000041

根据图4可以获得试样厚度与中心挠曲变形的关系式(11):According to Figure 4, the relationship between the thickness of the sample and the central deflection (11) can be obtained:

Figure BDA0001977865200000042
Figure BDA0001977865200000042

根据式(10)和(11)和试验数据,绘制试样厚度-试样中心挠曲变形的关系图,试验条件为425N时如图5所示。According to equations (10) and (11) and the test data, the relationship between the thickness of the sample and the deflection of the center of the sample is drawn, as shown in Figure 5 when the test condition is 425N.

第二步,根据Chakrabarty提出的小冲孔蠕变试验中等效蠕变应变与试样厚度之间的关系式,建立基于理想变形模型的等效蠕变应变与试样中心挠曲变形之间的关系式(12)In the second step, according to the relationship between the equivalent creep strain and the thickness of the specimen in the small punching creep test proposed by Chakrabarty, the relationship between the equivalent creep strain based on the ideal deformation model and the deflection deformation at the center of the specimen is established. Relation (12)

ε=ln(f(L)/0.5)=ln(2f(L)) (12)ε=ln(f(L)/0.5)=ln(2f(L)) (12)

利用式(10)-(12)绘制小冲杆蠕变试验中等效蠕变应变-(L/h0)的关系图,如图6所示。The equations (10)-(12) are used to draw the relationship diagram of the equivalent creep strain-(L/h 0 ) in the small punch creep test, as shown in Fig. 6 .

为了便于实际工程应用,利用式(13)进行拟合,得到不同材料小冲杆蠕变试验系数a,b,c,d,如表1所示。In order to facilitate practical engineering applications, equation (13) is used for fitting, and the creep test coefficients a, b, c, and d of small punches with different materials are obtained, as shown in Table 1.

ε=a(L/h0)4+b(L/h0)3+c(L/h0)2+d(L/h0) (13)ε=a(L/h 0 ) 4 +b(L/h 0 ) 3 +c(L/h 0 ) 2 +d(L/h 0 ) (13)

表1小冲杆蠕变试验参数值Table 1 Small punch creep test parameter values

Figure BDA0001977865200000051
Figure BDA0001977865200000051

第三步,利用上一步式关系式(13)耦合入如图2所示的小冲孔蠕变试验数据中(利用代入法进行耦合,一个数据对应一个结果,拟合出曲线后,再从该曲线中读取数据),得到Sanicro25钢在700℃不同载荷条件下的蠕变应变,与有限元分析得到的蠕变应变进行对比,如图7所示。可以发现本发明能够简便、较高精度地计算得到小冲孔蠕变试验中的蠕变应变,物理意义明确,具有更强的操作性和说服力。In the third step, use the relationship (13) of the previous step to couple into the small punching creep test data shown in Figure 2 (coupling is performed by the substitution method, one data corresponds to one result, after fitting the curve, and then from The data read in this curve), the creep strain of Sanicro25 steel under different load conditions at 700 °C is obtained, and the creep strain obtained by the finite element analysis is compared, as shown in Figure 7. It can be found that the invention can simply and accurately calculate the creep strain in the small punching creep test, has clear physical meaning, and has stronger operability and persuasion.

Claims (4)

1. A creep strain calculation method of a material under a small punch creep test is characterized by comprising the following steps:
step 1, analyzing deformation rules of different materials in a small punch creep process, dividing a small punch sample into three deformation regions, namely a spherical region a, a conical region b with unequal wall thickness and a region c with equal wall thickness, and establishing theoretical deformation model relational expressions (1) - (3) based on test conditions;
Figure FDA0001977865190000011
Figure FDA0001977865190000012
VC=π[R2-(R-A)2]h0(3)
in formulae (1), (2), and (3): vAVolume of the spherical region a, mm3,VBVolume of conical region b of unequal wall thickness, mm3,VCIs the volume of the region c with equal wall thickness, mm3R is the punching radius, mm; h isminIs the minimum thickness of the sample in mm, α is the included angle between the central line of the sample and the lower surface of the sample in DEG, h0Is the initial specimen thickness, mm; a is the width of the equal wall thickness area c, mm; r is the radius of the sample, mm;
step 2, establishing relational expressions (5) and (6) between small punching creep test center deflection deformation-included angle between sample center and deformation area and sample thickness-center deflection deformation by using the expression (4) according to the volume invariance principle in the sample deformation process; the corresponding relation between the thickness of the sample and the central deflection deformation of the sample, namely h, is established by using the formulas (5) and (6) and test datamin=f(L);
VA+VB+VC=πR2h0(4)
Figure FDA0001977865190000013
Figure FDA0001977865190000014
In the formula: l is the deflection deformation of the center of the sample collected in the test process, and is mm;
step 3, utilizing a relation (7) between equivalent creep strain and sample thickness in a small punch creep test proposed by Chakrabarty:
=ln(h0/hmin) (7)
in the formula: equivalent creep strain of a small punch test sample without dimensional parameters;
due to hminEstablishing a relation (8) between equivalent creep strain and sample center flexural deformation based on an ideal deformation model;
=ln(h0/f(L)) (8)
step 4, coupling the relational expressions (5), (6) and (8) obtained in the steps 2 and 3 into central deflection deformation data collected in a small punch creep test to obtain a corresponding relation between creep strain of the small punch creep test and sample central deflection deformation; in order to facilitate practical engineering application, the formula (9) is adopted to carry out nonlinear fitting to obtain important physical parameters a, b, c and d in a creep strain and center deflection deformation relational expression in a small punching creep test, and a creep strain and center deflection deformation relational expression in the small punching creep test is established;
=a(L/h0)4+b(L/h0)3+c(L/h0)2+d(L/h0) (9)
and 5, coupling the formula (9) into central deflection deformation-time curve data directly obtained by the small punch creep test, and finally establishing a relation graph of creep strain and test time of the small punch creep test.
2. Use of the material of claim 1 in creep strain calculation under small punch creep test to evaluate the remaining life of a service material during creep.
3. Use according to claim 2, wherein the service material is Sanicro25 austenitic stainless steel.
4. The application of claim 2, wherein the service temperature of the service material is 500-100 ℃.
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