CN108458930A - The method for determining material creep parameter with clamped straight-bar small sample creep test - Google Patents
The method for determining material creep parameter with clamped straight-bar small sample creep test Download PDFInfo
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Abstract
Description
技术领域technical field
本发明涉及材料蠕变,具体涉及一种运用固支直杆小试样蠕变试验确定材料蠕变参数的方法。The invention relates to material creep, in particular to a method for determining material creep parameters by using a fixed-supported straight bar small sample creep test.
背景技术Background technique
蠕变,也称潜变,是在应力影响下固体材料缓慢永久性的移动或者变形的趋势。它的发生是低于材料屈服强度的应力长时间作用的结果。当材料长时间处于加热当中或者在熔点附近时,蠕变会更加剧烈。蠕变常常随着温度升高而加剧。这种变形的速率与材料性质、加载时间、加载温度和加载结构应力有关。Creep, also called creep, is the tendency of a solid material to slowly and permanently move or deform under the influence of stress. It occurs as a result of prolonged stress below the yield strength of the material. Creep will be more severe when the material is heated for a long time or near the melting point. Creep often increases with increasing temperature. The rate of this deformation is related to material properties, loading time, loading temperature and loading structural stress.
在化工过程与发电行业,为了获得高的能源利用率,设备与构件的工作温度与工作压力不断提高,工作环境愈加严苛。为了保证设备与构件高效安全运行,对在役设备与构件的蠕变性能检测就显得必不可少。In the chemical process and power generation industries, in order to obtain high energy utilization, the working temperature and working pressure of equipment and components are constantly increasing, and the working environment is becoming more and more harsh. In order to ensure the efficient and safe operation of equipment and components, it is essential to detect the creep performance of in-service equipment and components.
蠕变试验,即测定金属材料在长时间的恒温和恒应力作用下,发生缓慢的塑性变形现象的一种材料机械性能试验。温度越高或应力越大,蠕变现象越显著。然而,传统单轴蠕变试样体积较大,取样会对设备造成较大损伤,有些设备与构件因体积较小,甚至无法提供试验所需的材料,这些促进了小试样蠕变方法的发展。Creep test is a kind of material mechanical performance test to determine the slow plastic deformation of metal materials under the action of constant temperature and constant stress for a long time. The higher the temperature or the greater the stress, the more significant the creep phenomenon. However, the volume of the traditional uniaxial creep specimen is large, and sampling will cause great damage to the equipment. Some equipment and components cannot even provide the materials required for the test due to their small volume. These promote the development of the small specimen creep method. develop.
固支直杆小试样蠕变试验,即采用固支直杆小试样来测试材料蠕变性能的试验方法,因其试验设备简易、试样受力简单、能够获得断裂数据等优点,具有比较大的研究价值。The creep test of small specimens supported by straight rods is a test method that uses small specimens supported by straight rods to test the creep properties of materials. Relatively large research value.
关于运用固支直杆小试样蠕变试验确定材料蠕变参数,目前研究多集中在基于小变形假设的梁弯曲理论,然而小变形假设与实际蠕变中常出现的大变形现象不符,因此,采用基于小变形假设的梁弯曲理论确定材料大变形阶段的蠕变参数在理论假设基础上存在不足,不适合用来确定固支直杆小试样的蠕变参数,需要建立新型的运用固支直杆小试样蠕变试验确定材料蠕变参数的方法。Regarding the determination of material creep parameters by the creep test of small specimens supported by fixed straight rods, the current research is mostly focused on the beam bending theory based on the assumption of small deformation. However, the assumption of small deformation is inconsistent with the phenomenon of large deformation that often occurs in actual creep. Therefore, Using the beam bending theory based on the assumption of small deformation to determine the creep parameters of materials in the stage of large deformation has insufficient theoretical assumptions. A method for determining the creep parameters of materials by creep tests on small straight rod specimens.
发明内容Contents of the invention
本发明的目的是提供一种运用固支直杆小试样蠕变试验确定材料蠕变参数的方法,本发明通过对材料不同变形阶段采用不同的蠕变变形理论分析,可以准确确定材料的蠕变参数,用以解决目前通过小变形假设的梁弯曲理论来确定材料大变形阶段的蠕变参数,使得材料蠕变参数的确定不够准确的问题。The purpose of the present invention is to provide a method for determining the creep parameters of a material by using the creep test of a small sample of a fixed straight rod. The present invention can accurately determine the creep of the material by using different creep deformation theories for different deformation stages of the material. The variable parameters are used to solve the problem that the creep parameters of the material in the large deformation stage are determined by the beam bending theory based on the small deformation assumption, which makes the determination of the material creep parameters not accurate enough.
为实现上述目的,本发明的方案是:一种运用固支直杆小试样蠕变试验确定材料蠕变参数的方法,所述方法步骤如下:In order to achieve the above object, the solution of the present invention is: a method for determining the creep parameters of a material by using the creep test of a small sample of a fixed straight rod, and the steps of the method are as follows:
步骤(1),对待确定蠕变参数的材料制作固支直杆小试样,进行固支直杆小试样蠕变试验,获取直杆小试样的蠕变位移-时间曲线;Step (1), making a small straight rod sample with a fixed support for the material whose creep parameters are to be determined, performing a creep test on the small straight rod sample with a fixed support, and obtaining the creep displacement-time curve of the small straight rod sample;
步骤(2),根据误差函数和直杆小试样的等效标距,确定直杆小试样发生小变形的临界位移,并根据直杆小试样的等效标距确定直杆小试样发生大变形的临界位移;Step (2), according to the error function and the equivalent gauge length of the small straight-bar sample, determine the critical displacement of the small deformation of the straight-bar small sample, and determine the straight-bar small test according to the equivalent gauge length of the straight-bar small sample The critical displacement of large deformation occurs;
步骤(3),根据直杆小试样发生小变形和大变形的临界位移,将得到的蠕变位移-时间曲线划分小变形阶段和大变形阶段;Step (3), divide the obtained creep displacement-time curve into a small deformation stage and a large deformation stage according to the critical displacement of small deformation and large deformation of the small straight rod sample;
步骤(4),根据步骤(3),确定直杆小试样发生稳态蠕变时所处的变形阶段;Step (4), according to step (3), determine the deformation stage when the steady-state creep of the small straight rod sample occurs;
步骤(5),当稳态蠕变发生在小变形阶段时,采用梁弯曲理论力学模型,对小变形阶段的蠕变位移-时间曲线进行分析,确定直杆小试样在小变形阶段的蠕变参数,该小变形阶段的蠕变参数即为材料的真实蠕变参数;Step (5), when the steady-state creep occurs in the small deformation stage, the beam bending theoretical mechanical model is used to analyze the creep displacement-time curve in the small deformation stage, and determine the creep of the small straight rod sample in the small deformation stage. The creep parameter in the small deformation stage is the real creep parameter of the material;
步骤(6),当稳态蠕变发生在大变形阶段时,采用全局变形理论力学模型,对大变形阶段的蠕变位移-时间曲线进行分析,确定直杆小试样在大变形阶段的蠕变参数,该大变形阶段的蠕变参数即为材料的真实蠕变参数。Step (6), when the steady-state creep occurs in the large deformation stage, use the global deformation theoretical mechanical model to analyze the creep displacement-time curve in the large deformation stage, and determine the creep of the small straight rod sample in the large deformation stage The creep parameter of the large deformation stage is the real creep parameter of the material.
本发明对蠕变位移-时间曲线进行了不同变形阶段的划分,通过判断材料发生稳态蠕变所处的变形阶段,对不同的变形阶段采用不同的理论模型进行分析,确定材料的蠕变参数,结果更加真实准确可靠。The invention divides the creep displacement-time curve into different deformation stages, and by judging the deformation stage where the steady-state creep of the material occurs, different theoretical models are used to analyze the different deformation stages to determine the creep parameters of the material , the result is more realistic, accurate and reliable.
进一步地,根据本发明所述的运用固支直杆小试样蠕变试验确定材料蠕变参数方法,其特征在于:步骤(2)中所述的误差函数为:Further, according to the method of determining the creep parameters of the material by using the creep test of the fixed straight rod small sample according to the present invention, it is characterized in that: the error function described in the step (2) is:
其中,Φ为误差函数,x为试样轴线方向的长度变量,d为试样中心蠕变位移,θ为试样的截面转角。Among them, Φ is the error function, x is the length variable in the axial direction of the sample, d is the creep displacement of the sample center, and θ is the section rotation angle of the sample.
进一步地,根据本发明所述的运用固支直杆小试样蠕变试验确定材料蠕变参数方法,所述的步骤(2)中,小变形的临界位移为:Further, according to the method of determining the material creep parameters by using the creep test of the fixed straight rod small sample according to the present invention, in the described step (2), the critical displacement of the small deformation is:
其中,dcs为小变形的临界位移,l为梁下支点间的整体长度,θmax为误差函数达到0.1时的临界转角。Among them, d cs is the critical displacement of small deformation, l is the overall length between the lower fulcrums of the beam, and θ max is the critical rotation angle when the error function reaches 0.1.
进一步地,根据本发明所述的运用固支直杆小试样蠕变试验确定材料蠕变参数方法,所述的步骤(2)中,大变形的临界位移为:Further, according to the method of determining material creep parameters by using the creep test of a small sample of a fixed straight rod according to the present invention, in the described step (2), the critical displacement of large deformation is:
dcl=0.2·l dcl = 0.2·l
其中,dcl为大变形的临界位移,l为梁下支点间的整体长度。Among them, d cl is the critical displacement of large deformation, and l is the overall length between the lower fulcrums of the beam.
进一步地,根据本发明所述的运用固支直杆小试样蠕变试验确定材料蠕变参数方法,步骤(5)中所述的梁弯曲理论力学模型为:Further, according to the method of determining the material creep parameters by using the creep test of the fixed straight bar small sample according to the present invention, the beam bending theoretical mechanical model described in step (5) is:
其中,为试样中心蠕变位移速率,b为试样的宽度,2h为试样的原始厚度,P为试样蠕变载荷,l为梁下支点间的整体长度,n为材料的指数参数,B为材料常数,σeq'为小变形阶段的等效应力,为小变形阶段的等效应变速率。in, is the creep displacement rate at the center of the sample, b is the width of the sample, 2h is the original thickness of the sample, P is the creep load of the sample, l is the overall length between the lower fulcrums of the beam, n is the index parameter of the material, B is the material constant, σ eq ' is the equivalent stress in the stage of small deformation, is the equivalent strain rate in the small deformation stage.
本发明对现有的梁弯曲理论力学模型进行了修正,修正的梁弯曲理论力学模型考虑了试样的整体变形长度,与单轴蠕变关联性更好。The present invention modifies the existing theoretical mechanical model of beam bending, and the modified theoretical mechanical model of beam bending takes into account the overall deformation length of the sample, and has better correlation with uniaxial creep.
进一步地,根据本发明所述的运用固支直杆小试样蠕变试验确定材料蠕变参数方法,步骤(6)中所述的全局变形理论力学模型为:Further, according to the method of determining the material creep parameters by using the creep test of the fixed straight rod small sample according to the present invention, the global deformation theoretical mechanical model described in step (6) is:
其中,d为试样中心蠕变位移,R为试验压头半径,θ0为压头与试样接触的最大转角,l为梁下支点间的整体长度,εeq为大变形阶段的整体等效应变,σeq为大变形阶段的等效应力,P为试样蠕变载荷,大变形阶段的整体等效应变速率。Among them, d is the creep displacement of the sample center, R is the radius of the test indenter, θ0 is the maximum contact angle between the indenter and the sample, l is the overall length between the lower fulcrums of the beam, ε eq is the overall length of the large deformation stage, etc. effect strain, σ eq is the equivalent stress in the stage of large deformation, P is the creep load of the specimen, The overall equivalent strain rate for the large deformation stage.
进一步地,根据本发明所述的运用固支直杆小试样蠕变试验确定材料蠕变参数方法,所述步骤(5)中,对所述的蠕变位移-时间曲线进行微分处理,获得蠕变位移速率-时间曲线,并根据蠕变位移速率-时间曲线确定材料的稳态蠕变位移速率,将所述的稳态蠕变位移速率与载荷代入梁弯曲理论力学模型,获得直杆小试样小变形阶段的等效应力与等效应变速率,并绘制双对数坐标下试样的稳态应变速率-等效应力关系曲线,并通过对稳态应变速率-等效应力关系曲线进行线性拟合,得到材料的蠕变参数。Further, according to the method of determining the creep parameters of the material by using the creep test of the fixed straight rod small sample according to the present invention, in the step (5), the described creep displacement-time curve is differentially processed to obtain creep displacement rate-time curve, and determine the steady-state creep displacement rate of the material according to the creep displacement rate-time curve, and substitute the steady-state creep displacement rate and load into the beam bending theoretical mechanical model to obtain the straight rod small The equivalent stress and equivalent strain rate of the sample in the small deformation stage, and draw the steady-state strain rate-equivalent stress relationship curve of the sample under the double-logarithmic coordinates, and through the steady-state strain rate-equivalent stress relationship curve Linear fitting to obtain the creep parameters of the material.
进一步地,根据本发明所述的运用固支直杆小试样蠕变试验确定材料蠕变参数方法,所述步骤(6)中,根据所述的蠕变位移-时间曲线确定稳态蠕变位移,并将所述的稳态蠕变位移与载荷代入全局变形理论力学模型,得到大变形阶段的等效应变与等效应力,并将等效应变对时间进行微分,得到直杆小试样大变形阶段的等效应变速率,并绘制双对数坐标下试样的稳态应变速率-等效应力关系曲线,并通过对稳态应变速率-等效应力关系曲线进行线性拟合,得到材料的蠕变参数。Further, according to the method for determining the material creep parameters by using the creep test of the fixed straight rod small sample according to the present invention, in the step (6), the steady-state creep is determined according to the creep displacement-time curve Displacement, and the steady-state creep displacement and load are substituted into the global deformation theoretical mechanical model to obtain the equivalent strain and equivalent stress in the large deformation stage, and the equivalent strain is differentiated with respect to time to obtain a straight rod small sample The equivalent strain rate in the large deformation stage, and draw the steady-state strain rate-equivalent stress relationship curve of the sample in log-logarithmic coordinates, and through linear fitting of the steady-state strain rate-equivalent stress relationship curve, the material creep parameters.
本发明达到的有益效果:(1)本发明通过计算固支直杆小试样发生小变形与大变形的临界位移,将蠕变位移-时间曲线划分出大变形阶段和小变形阶段,不同的蠕变变形阶段的蠕变变形采用不同的理论分析方法,使得获取的蠕变参数更加准确。The beneficial effects that the present invention reaches: (1) the present invention divides the creep displacement-time curve into a large deformation stage and a small deformation stage by calculating the critical displacement of small deformation and large deformation of a small sample of fixed straight rod, different Different theoretical analysis methods are used for creep deformation in the creep deformation stage, so that the obtained creep parameters are more accurate.
(2)本发明对稳态蠕变发生在小变形阶段时的力学模型进行了修正,与有效跨距法相比,修正的梁弯曲理论模型考虑了试样的真实跨距,与单轴蠕变关联性更好。(2) The present invention has revised the mechanical model when the steady-state creep occurs in the small deformation stage. Compared with the effective span method, the corrected beam bending theoretical model has considered the true span of the sample, and is different from the uniaxial creep method. Relevance is better.
(3)本发明对稳态蠕变发生在大变形阶段时的力学模型进行了研究,基于全局变形理论提出了固支蠕变大变形阶段的分析方法,可以获得材料大变形下的蠕变变形参数。(3) The present invention studies the mechanical model of steady-state creep occurring in the large deformation stage, and proposes an analysis method for anchored creep in the large deformation stage based on the global deformation theory, which can obtain the creep deformation of the material under large deformation parameter.
附图说明Description of drawings
图1为固支直杆小试样蠕变参数确定方法的流程图。Fig. 1 is a flow chart of the method for determining the creep parameters of small straight rod specimens.
图2为固支直杆小试样蠕变试验的安装示意图。Figure 2 is a schematic diagram of the installation of the creep test of a small sample on a fixed straight rod.
图3为固支直杆小试样蠕变试验装置。Figure 3 is a creep test device for a small straight rod sample.
图4为380℃下A7N01铝合金的固支直杆小试样蠕变位移时间曲线。Fig. 4 is the creep displacement time curve of a small sample of a fixed straight rod of A7N01 aluminum alloy at 380°C.
图5为A7N01铝合金固支直杆小试样蠕变位移-时间曲线变形阶段的划分。Figure 5 shows the division of the deformation stages of the creep displacement-time curve of a small sample of A7N01 aluminum alloy fixed straight rod.
图6为基于小变形假设的梁弯曲理论力学模型。Fig. 6 is the theoretical mechanical model of beam bending based on the assumption of small deformation.
图7为基于大变形假设的全局变形理论力学模型。Fig. 7 is a theoretical mechanical model of global deformation based on the assumption of large deformation.
图8为380℃下A7N01铝合金的单轴蠕变试验曲线。Figure 8 is the uniaxial creep test curve of A7N01 aluminum alloy at 380°C.
图9为不同变形理论下A7N01铝合金的等效应力与等效应变速率的关系。Figure 9 shows the relationship between the equivalent stress and the equivalent strain rate of the A7N01 aluminum alloy under different deformation theories.
图中,1为夹具上模,2为夹具下模,3为压头,4为直杆小试样。In the figure, 1 is the upper mold of the fixture, 2 is the lower mold of the fixture, 3 is the indenter, and 4 is a small straight rod sample.
具体实施方式Detailed ways
下面结合附图和具体的实施例对本发明作进一步详细的说明。The present invention will be described in further detail below in conjunction with the accompanying drawings and specific embodiments.
本发明的方法如下:Method of the present invention is as follows:
(1)本发明运用固支直杆小试样蠕变试验获取材料的蠕变位移-时间曲线,并将蠕变位移-时间曲线划分为小变形阶段、过渡阶段与大变形阶段。(1) The present invention obtains the creep displacement-time curve of the material by using the creep test of a small straight bar sample, and divides the creep displacement-time curve into a small deformation stage, a transition stage and a large deformation stage.
本发明中的固支直杆小试样蠕变试验满足《GB/T2039-2012金属材料单轴拉伸试验方法》规定的蠕变试验条件。The creep test of the fixed-supported straight bar small sample in the present invention meets the creep test conditions stipulated in "GB/T2039-2012 Metal Material Uniaxial Tensile Test Method".
(2)通过直杆小试样发生小变形和大变形的临界位移,对直杆小试样发生稳态蠕变所处的变形阶段进行分析判断;(2) Analyzing and judging the deformation stage of the steady-state creep of the straight rod small sample through the critical displacement of small deformation and large deformation of the straight rod small sample;
(3)当稳态蠕变发生在小变形阶段时,采用梁弯曲理论力学模型进行分析,获取材料小变形阶段的蠕变参数,并将该小变形阶段的蠕变参数作为材料的真实蠕变参数。具体为:(3) When the steady-state creep occurs in the small deformation stage, the beam bending theoretical mechanical model is used for analysis to obtain the creep parameters in the small deformation stage of the material, and the creep parameters in the small deformation stage are taken as the real creep of the material parameter. Specifically:
将步骤(1)得到的蠕变位移-时间曲线进行微分处理,获得蠕变位移速率-时间曲线,蠕变位移速率-时间曲线中,蠕变位移速率随时间变化缓慢或几乎无变化时,所对应的蠕变位移速率为相应载荷下的稳态蠕变位移速率,将所述的稳态蠕变位移速率与载荷代入梁弯曲理论力学模型,得到直杆小试样梁弯曲理论下的等效应力与稳态应变速率,将稳态应变速率和等效应力绘于双对数坐标下,得到稳态应变速率-等效应力关系曲线,并对稳态应变速率-等效应力曲线进行线性拟合,得到梁弯曲理论下小变形阶段的蠕变参数B、n,即为材料的真实蠕变参数。Differentiate the creep displacement-time curve obtained in step (1) to obtain the creep displacement rate-time curve. In the creep displacement rate-time curve, when the creep displacement rate changes slowly or hardly changes with time, the The corresponding creep displacement rate is the steady-state creep displacement rate under the corresponding load, and the above-mentioned steady-state creep displacement rate and load are substituted into the beam bending theoretical mechanical model to obtain the equivalent effect under the beam bending theory of the straight rod small sample Stress and steady-state strain rate, draw the steady-state strain rate and equivalent stress on the log-logarithmic coordinates, obtain the steady-state strain rate-equivalent stress relationship curve, and perform linear fitting on the steady-state strain rate-equivalent stress curve Combined, the creep parameters B and n in the small deformation stage under the beam bending theory are obtained, which are the real creep parameters of the material.
本发明采用的梁弯曲理论力学模型为:The beam bending theoretical mechanics model that the present invention adopts is:
其中,为蠕变位移速率,b为试样的宽度,2h为试样的原始厚度,P为试样蠕变载荷,l为梁下支点间的整体长度,n为材料的指数参数,B为材料常数,σeq'为小变形阶段的等效应力,为小变形阶段的等效应变速率。in, is the creep displacement rate, b is the width of the sample, 2h is the original thickness of the sample, P is the creep load of the sample, l is the overall length between the lower fulcrums of the beam, n is the index parameter of the material, and B is the material constant , σ eq ' is the equivalent stress in the stage of small deformation, is the equivalent strain rate in the small deformation stage.
(4)当稳态蠕变发生在大变形阶段时,采用全局变形理论力学模型进行分析,获取材料大变形阶段的蠕变参数,并将该大变形阶段的蠕变参数作为材料的真实蠕变参数。具体为:(4) When the steady-state creep occurs in the large deformation stage, the global deformation theoretical mechanical model is used for analysis to obtain the creep parameters in the large deformation stage of the material, and the creep parameters in the large deformation stage are taken as the real creep of the material parameter. Specifically:
根据步骤(1)得到的载荷、蠕变位移与时间代入全局变形理论力学模型,得到大变形阶段的等效应变-时间曲线以及等效应力-时间曲线,将等效应变-时间曲线进行微分处理,得到全局变形理论下的等效应变速率-时间曲线,并确定全局变形理论下试样的稳态应变速率与对应的等效应力,将稳态应变速率和等效应力绘于双对数坐标下,得到稳态应变速率-等效应力关系曲线,如图9所示,在双对数坐标下,稳态应变速率与等效应力呈现线性关系,对图9的稳态应变速率-等效应力曲线进行线性拟合,得到全局变形理论下大变形阶段的蠕变参数B、n,即为材料的真实蠕变参数。Substitute the load, creep displacement and time obtained in step (1) into the global deformation theoretical mechanical model to obtain the equivalent strain-time curve and equivalent stress-time curve in the large deformation stage, and perform differential processing on the equivalent strain-time curve , obtain the equivalent strain rate-time curve under the global deformation theory, and determine the steady-state strain rate and corresponding equivalent stress of the sample under the global deformation theory, and plot the steady-state strain rate and equivalent stress on the logarithmic coordinate , the steady-state strain rate-equivalent stress relationship curve is obtained, as shown in Figure 9, under the log-logarithmic coordinates, the steady-state strain rate and the equivalent stress present a linear relationship, and the steady-state strain rate-equivalent stress in Figure 9 The force curve is linearly fitted to obtain the creep parameters B and n in the large deformation stage under the global deformation theory, which are the real creep parameters of the material.
本发明采用的全局变形理论力学模型为:The global deformation theory mechanics model that the present invention adopts is:
其中,d为试样中心蠕变位移,R为试验压头半径,θ0为压头与试样接触的最大转角,l为梁下支点间的整体长度,εeq为大变形阶段的整体等效应变,σeq为大变形阶段的等效应力,P为试样蠕变载荷,大变形阶段的整体等效应变速率。Among them, d is the creep displacement of the sample center, R is the radius of the test indenter, θ0 is the maximum contact angle between the indenter and the sample, l is the overall length between the lower fulcrums of the beam, ε eq is the overall length of the large deformation stage, etc. effect strain, σ eq is the equivalent stress in the stage of large deformation, P is the creep load of the specimen, The overall equivalent strain rate for the large deformation stage.
实施例:材料为A7N01铝合金,固支直杆小试样的试验温度为380℃,运用本发明的方法确定A7N01铝合金蠕变参数的过程如下:Embodiment: The material is A7N01 aluminum alloy, and the test temperature of the small straight rod sample fixedly supported is 380°C. The process of using the method of the present invention to determine the creep parameters of A7N01 aluminum alloy is as follows:
1,对A7N01铝合金取材,并制作A7N01铝合金的固支直杆小试样,如图2,用夹具上模1固定直杆小试样4的两端,压头3下端压紧直杆小试样4的中间区域,在380℃下对A7N01铝合金进行不同蠕变载荷的蠕变试验,并在试验结束后,获取并记录直杆试样的蠕变位移-时间曲线,如图4所示。1. Take materials from A7N01 aluminum alloy, and make a small straight rod sample of A7N01 aluminum alloy. In the middle area of small sample 4, creep tests were carried out on A7N01 aluminum alloy with different creep loads at 380°C, and after the test, the creep displacement-time curve of the straight rod sample was obtained and recorded, as shown in Figure 4 shown.
2,通过误差函数,结合试验装置的尺寸,确定试样发生小变形与大变形的临界位移分别为1.003mm与2.40mm。2. Through the error function, combined with the size of the test device, it is determined that the critical displacement of the sample for small deformation and large deformation is 1.003mm and 2.40mm respectively.
本实施例的误差函数为:The error function of this embodiment is:
其中,Φ为误差函数,x为试样的轴线方向,d为试样中心蠕变位移,θ为试样的截面转角。Among them, Φ is the error function, x is the axial direction of the sample, d is the creep displacement of the sample center, and θ is the section rotation angle of the sample.
小变形的临界位移计算方法为:大变形的临界位移计算方法为:dcl=0.2·l。其中,l为梁下支点间的整体长度,即试验装置的夹具下模之间的跨距,θmax为误差函数达到0.1时的临界转角。The critical displacement calculation method for small deformation is: The critical displacement calculation method for large deformation is: d cl =0.2·l. Among them, l is the overall length between the lower fulcrums of the beam, that is, the span between the lower dies of the fixture of the test device, and θ max is the critical rotation angle when the error function reaches 0.1.
3,根据试样发生小变形与大变形的临界位移,将得到的蠕变位移-时间曲线划分为小变形阶段、过渡阶段与大变形阶段,如图5所示,从图5可以确定,本实施例中,试样的稳态蠕变发生在大变形阶段。3. According to the critical displacement of small deformation and large deformation of the sample, the obtained creep displacement-time curve is divided into small deformation stage, transition stage and large deformation stage, as shown in Figure 5. It can be determined from Figure 5 that this In the example, the steady-state creep of the sample occurs in the stage of large deformation.
4,因为稳态蠕变发生在大变形阶段,采用全局变形理论力学模型,对图5中大变形阶段的蠕变位移-时间曲线进行分析,按照上述(4)的方法,确定大变形阶段的蠕变参数,本实施例得到的蠕变参数为B=2.381E-9,n=5.80。4. Since the steady-state creep occurs in the large deformation stage, the global deformation theoretical mechanical model is used to analyze the creep displacement-time curve in the large deformation stage in Fig. 5, and the large deformation stage is determined according to the above method (4). Creep parameters, the creep parameters obtained in this embodiment are B=2.381E-9, n=5.80.
5,将全局变形理论得到材料蠕变参数作为材料的真实蠕变参数。5. Use the material creep parameters obtained from the global deformation theory as the real creep parameters of the material.
将本实施例中运用本发明方法确定的蠕变参数与单轴蠕变试验得到的蠕变参数进行比较,如图8所示为单轴蠕变试验的曲线,单轴蠕变试验得到的蠕变参数为B=1.988E-9,n=5.75。可见,本发明方法确定的蠕变参数与单轴蠕变得到的蠕变参数非常接近,运用本发明方法确定的材料蠕变参数比较准确,图9为单轴蠕变与本实施例固支直杆蠕变试验条件下A7N01铝合金的等效应力与等效应变速率的关系。In this embodiment, the creep parameter determined by the method of the present invention is compared with the creep parameter obtained by the uniaxial creep test, as shown in Figure 8, it is the curve of the uniaxial creep test, and the creep parameter obtained by the uniaxial creep test The variable parameters are B=1.988E-9, n=5.75. It can be seen that the creep parameters determined by the method of the present invention are very close to the creep parameters obtained by uniaxial creep, and the creep parameters of materials determined by the method of the present invention are relatively accurate. The relationship between equivalent stress and equivalent strain rate of A7N01 aluminum alloy under rod creep test conditions.
本发明通过计算直杆小试样发生小变形与大变形的临界位移,将蠕变位移-时间曲线划分出大变形阶段和小变形阶段,不同的蠕变变形阶段的蠕变变形采用不同的理论分析方法:当稳态蠕变发生在小变形阶段时,采用梁弯曲理论分析,获取材料的蠕变参数;当稳态蠕变发生在大变形阶段时,采用全局变形理论进行分析,获取材料的蠕变参数。不同变形阶段采用不同的理论分析方法,使得获取的蠕变参数更加准确、真实。The present invention divides the creep displacement-time curve into a large deformation stage and a small deformation stage by calculating the critical displacement of small deformation and large deformation of a small straight rod sample, and different theories are adopted for the creep deformation of different creep deformation stages Analysis method: when the steady-state creep occurs in the small deformation stage, the beam bending theory is used to obtain the creep parameters of the material; when the steady-state creep occurs in the large deformation stage, the global deformation theory is used for analysis to obtain the material's Creep parameter. Different theoretical analysis methods are adopted in different deformation stages, so that the obtained creep parameters are more accurate and real.
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