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CN113702613B - A method for determining critical conditions for dynamic recrystallization of materials - Google Patents

A method for determining critical conditions for dynamic recrystallization of materials Download PDF

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CN113702613B
CN113702613B CN202110956655.6A CN202110956655A CN113702613B CN 113702613 B CN113702613 B CN 113702613B CN 202110956655 A CN202110956655 A CN 202110956655A CN 113702613 B CN113702613 B CN 113702613B
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赵宝纯
黄磊
王英海
马惠霞
胡筱旋
王婷
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Angang Steel Co Ltd
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Abstract

The invention relates to a method for determining critical conditions for dynamic recrystallization of a material, comprising: 1) Carrying out a single compression experiment on the experimental material to obtain a stress-strain curve in the deformation process; 2) Taking absolute values of stress sigma and strain epsilon data, and then redrawing a stress-strain curve in a sigma-lg epsilon semi-logarithmic coordinate system or in a lg sigma-lg epsilon double-logarithmic coordinate system; 3) Calibrating the linear section part interval, and selecting different subintervals to perform multiple linear regression; selecting a linear regression equation obtained from subintervals with regression coefficients R more than or equal to 0.99; 4) Drawing xi in rectangular coordinate system 2 -epsilon curve; 5) The critical strain value at which dynamic recrystallization of the material occurs is determined. The invention can rapidly and accurately determine the critical condition of dynamic recrystallization of the material during compression deformation, and provides a basis for grasping the technological parameters of the steel material during the hot working process and optimizing the hot working process.

Description

一种确定材料发生动态再结晶临界条件的方法A method for determining critical conditions for dynamic recrystallization of materials

技术领域Technical field

本发明涉及金属材料热加工技术领域,尤其涉及一种确定材料发生动态再结晶临界条件的方法。The present invention relates to the technical field of thermal processing of metal materials, and in particular to a method for determining critical conditions for dynamic recrystallization of materials.

背景技术Background technique

金属材料在高温塑性变形时,一方面会随变形量的增加产生加工硬化,使材料内部产生大量的位错;另一方面同时会产生动态回复和动态再结晶的软化过程以抵消此加工硬化。动态再结晶对随后的相变行为和最终产品的力学性能影响很大,目前关于研究金属和合金在热变形过程动态再结晶的数学模型工作之一是确定发生动态再结晶的临界条件。When metal materials are plastically deformed at high temperatures, on the one hand, work hardening will occur as the amount of deformation increases, causing a large number of dislocations inside the material; on the other hand, the softening process of dynamic recovery and dynamic recrystallization will occur to offset this work hardening. Dynamic recrystallization has a great influence on the subsequent phase transformation behavior and the mechanical properties of the final product. One of the current mathematical modeling efforts to study the dynamic recrystallization of metals and alloys during hot deformation is to determine the critical conditions for dynamic recrystallization to occur.

最初,一些学者把材料真应力-应变曲线中的峰值应力所对应的应变作为动态再结晶临界应变,之后研究发现金属在达到峰值应力之前就已经发生再结晶。因此,以应力峰值对应的应变为发生动态再结晶的临界应变是不合适的。另一种直接的方法是通过观察不同应变量下的金相显微组织来确定动态再结晶临界应变,这种方法操作难度大,且所确定的临界应变与实际临界应变存在一定偏差。Initially, some scholars regarded the strain corresponding to the peak stress in the material's true stress-strain curve as the critical strain for dynamic recrystallization. Later studies found that the metal recrystallized before reaching the peak stress. Therefore, it is inappropriate to use the strain corresponding to the stress peak as the critical strain for dynamic recrystallization. Another direct method is to determine the critical strain of dynamic recrystallization by observing the metallographic microstructure under different strains. This method is difficult to operate, and there is a certain deviation between the determined critical strain and the actual critical strain.

专利号为ZL201811110795.6的中国发明专利公开了一种“预测微合金钢热轧时发生动态再结晶临界压下量的方法”,其是基于金相组织观察,通过对圆柱形试样在变形温度850~1250℃区间进行高温压缩实验,在实验获取的流变应力曲线上读取不同温度下的峰值应变,并计算出不同温度下发生动态再结晶临界应变的范围,两者结合起来确定发生动态再结晶的临界应变,然后通过线性拟合得到峰值应力对应的应变与临界应变的关系式。这种方法中选用的临界应变范围是一个较宽的数据区间,并且该区间也不能涵盖所有材料的流变行为特征,金相组织观察操作难度大,线性拟合也存在一定偏差,因此,该方法难于给出准确的临界应变。The Chinese invention patent with patent number ZL201811110795.6 discloses a "method for predicting the critical reduction of dynamic recrystallization during hot rolling of microalloy steel". It is based on the observation of metallographic structure and through the deformation of cylindrical samples. Conduct high-temperature compression experiments in the temperature range of 850 to 1250°C, read the peak strains at different temperatures on the flow stress curve obtained from the experiment, and calculate the range of critical strains for dynamic recrystallization at different temperatures. The two are combined to determine the occurrence of dynamic recrystallization. The critical strain of dynamic recrystallization is then obtained through linear fitting to obtain the relationship between the strain corresponding to the peak stress and the critical strain. The critical strain range selected in this method is a wide data interval, and this interval cannot cover the rheological behavior characteristics of all materials. It is difficult to observe the metallographic structure, and there is also a certain deviation in the linear fitting. Therefore, this interval The method is difficult to give accurate critical strain.

Ryan、McQueen和Kocks等根据动态回复和动态再结晶、应变硬化行为的差别,将θ-σ曲线上θ和σ开始偏离线性关系处的应力定义为临界应力,并从而确定临界应变。然而,当真应力小于临界应力时,θ和σ之间的线性关系并不是必然的,这就难于确定出拐点的位置,即临界应力。且获取θ-σ曲线,需要对实验数据进行拟合,微分以及曲线转化等操作。Based on the differences between dynamic recovery, dynamic recrystallization, and strain hardening behaviors, Ryan, McQueen, and Kocks defined the stress at which θ and σ on the θ-σ curve begin to deviate from the linear relationship as the critical stress, and thereby determined the critical strain. However, when the true stress is less than the critical stress, the linear relationship between θ and σ is not inevitable, which makes it difficult to determine the location of the inflection point, that is, the critical stress. And obtaining the θ-σ curve requires operations such as fitting, differentiation, and curve transformation of experimental data.

综上,为了快速、准确地确定出发生动态再结晶的临界条件,还需寻找一种新的确定方法。In summary, in order to quickly and accurately determine the critical conditions for dynamic recrystallization, a new determination method needs to be found.

发明内容Contents of the invention

本发明提供了一种确定材料发生动态再结晶临界条件的方法,能够快速、准确地确定材料在压缩变形时发生动态再结晶的临界条件,为掌握钢铁材料在热加工过程的工艺参数,优化热加工工艺提供基础。The present invention provides a method for determining the critical conditions for dynamic recrystallization of materials, which can quickly and accurately determine the critical conditions for dynamic recrystallization of materials during compression deformation. In order to master the process parameters of steel materials in the thermal processing process and optimize the thermal processing Processing technology provides the basis.

为了达到上述目的,本发明采用以下技术方案实现:In order to achieve the above objects, the present invention adopts the following technical solutions:

一种确定材料发生动态再结晶临界条件的方法,包括如下步骤:A method for determining critical conditions for dynamic recrystallization of materials, including the following steps:

1)通过热力模拟实验对实验材料进行单道次压缩实验,得到实验材料变形过程中的应力应变曲线;对得到的应力应变曲线进行平滑处理,去除噪声对实验曲线的影响;1) Conduct a single-pass compression experiment on the experimental material through a thermal simulation experiment to obtain the stress-strain curve during the deformation process of the experimental material; smooth the obtained stress-strain curve to remove the influence of noise on the experimental curve;

2)将与步骤1)中所述应力应变曲线相对应的应力σ和应变ε数据取绝对值,即应力σ和应变ε均为正值;然后在σ-lgε半对数坐标系或在lgσ-lgε双对数坐标系内重新绘制应力应变曲线;2) Take the absolute value of the stress σ and strain ε data corresponding to the stress strain curve described in step 1), that is, the stress σ and strain ε are both positive values; then in the σ-lgε semi-logarithmic coordinate system or in lgσ -Redraw the stress-strain curve in the lgε logarithmic coordinate system;

3)根据步骤2)重新绘制的应力应变曲线的形状特征,标定线性段部分区间,在其中选择不同的子区间进行多次线性回归;选择回归系数R≥0.99的子区间获得的线性回归方程,回归方程用如下公式表示:3) According to the shape characteristics of the stress-strain curve redrawn in step 2), calibrate some intervals of the linear segment, and select different sub-intervals to perform multiple linear regressions; select the linear regression equation obtained from the sub-interval with a regression coefficient R≥0.99, The regression equation is expressed by the following formula:

σ1=A+Blgε (1)σ 1 =A+Blgε (1)

lgσ2=A1+B1lgε (2)lgσ 2 =A 1 +B 1 lgε (2)

式中,σ1为应力值;lgσ2为应力值对数;A、B、A1、B1为回归系数;In the formula, σ 1 is the stress value; lgσ 2 is the logarithm of the stress value; A, B, A 1 and B 1 are regression coefficients;

若子区间在σ-lgε半对数坐标系下选取,则选用公式(1),若子区间在lgσ-lgε双对数坐标系下选取,则选用公式(2);If the subinterval is selected under the σ-lgε semi-logarithmic coordinate system, then formula (1) is used; if the subinterval is selected under the lgσ-lgε double logarithmic coordinate system, then formula (2) is used;

4)以步骤2)中所述应变ε为自变量,采用步骤3)所述公式(1)或公式(2)计算应力值σ1或应力值对数lgσ2,将所计算的应力值或应力值对数与步骤2)所述应力σ或lgσ进行比较,得到如下公式:4) Using the strain ε described in step 2) as the independent variable, use the formula (1) or formula (2) described in step 3) to calculate the stress value σ 1 or the logarithm of the stress value lgσ 2 , and calculate the stress value or Compare the logarithm of the stress value with the stress σ or lgσ described in step 2) to obtain the following formula:

ξ1=σ1-σ (3)ξ 11 -σ (3)

ξ2=lgσ2-lgσ (4)ξ 2 =lgσ 2 -lgσ (4)

式中,ξ1为在σ-lgε半对数坐标系下的特征应力差,ξ2为在lgσ-lgε双对数坐标系下由于特征应力差异导致的增量;In the formula, ξ 1 is the characteristic stress difference under the σ-lgε semi-logarithmic coordinate system, ξ 2 is the increment caused by the characteristic stress difference under the lgσ-lgε double logarithmic coordinate system;

若子区间在σ-lgε半对数坐标系下选取,则选用公式(3)计算出ξ1,并在直角坐标系下绘制ξ1-ε曲线;若子区间在lgσ-lgε双对数坐标系下选取,则选用公式(4)计算出ξ2,并在直角坐标系下绘制ξ2-ε曲线;If the subinterval is selected under the σ-lgε semi-logarithmic coordinate system, use formula (3) to calculate ξ 1 and draw the ξ 1 -ε curve under the rectangular coordinate system; if the subinterval is selected under the lgσ-lgε double logarithmic coordinate system If selected, use formula (4) to calculate ξ 2 and draw the ξ 2 -ε curve in the Cartesian coordinate system;

5)对步骤4)中获得的ξ1-ε曲线或ξ2-ε曲线进行分析,可知该曲线在选定的应变子区间内值为零;当应变超出所选应变子区间时,随着应变增大到某一个数值,计算值将大于实验值,该数值即为材料发生动态再结晶的临界应变值。5) Analyze the ξ 1 -ε curve or ξ 2 -ε curve obtained in step 4). It can be seen that the value of this curve is zero in the selected strain sub-interval; when the strain exceeds the selected strain sub-interval, as the When the strain increases to a certain value, the calculated value will be greater than the experimental value. This value is the critical strain value for dynamic recrystallization of the material.

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:

基于材料在变形过程中经历的加工硬化和回复软化以及动态再结晶软化等过程,通过对数坐标系凸显出发生动态再结晶对应力值的减小作用,通过曲线拟合找出与应力相关的特征计算值与实际值的差异,进而快速、准确地确定出发生动态再结晶的临界条件,为研究材料的动态再结晶过程奠定基础。Based on the process of work hardening, recovery softening and dynamic recrystallization softening experienced by the material during the deformation process, the reducing effect of dynamic recrystallization on the stress value is highlighted through the logarithmic coordinate system, and the stress-related stress values are found through curve fitting. The difference between the characteristic calculated value and the actual value can quickly and accurately determine the critical conditions for dynamic recrystallization, which lays the foundation for studying the dynamic recrystallization process of materials.

附图说明Description of the drawings

图1是实施例1中直角坐标系下实验钢在1000℃变形过程中的应力应变曲线。Figure 1 is the stress-strain curve of the experimental steel during deformation at 1000°C in the Cartesian coordinate system in Example 1.

图2是实施例1中σ-lgε半对数坐标系下实验钢在1000℃变形过程中的应力应变曲线。Figure 2 is the stress-strain curve of the experimental steel during deformation at 1000°C in the σ-lgε semi-logarithmic coordinate system in Example 1.

图3是实施例1中实验钢在1000℃变形应力应变曲线计算值与实验值对比图。Figure 3 is a comparison chart between the calculated values and experimental values of the deformation stress-strain curve of the experimental steel in Example 1 at 1000°C.

图3中,1为应力应变曲线计算值,2为应力应变曲线实验值。In Figure 3, 1 is the calculated value of the stress-strain curve, and 2 is the experimental value of the stress-strain curve.

图4是实施例1中实验钢在1000℃变形发生动态再结晶临界应变的确定示意图。Figure 4 is a schematic diagram for determining the critical strain of dynamic recrystallization of the experimental steel deformed at 1000°C in Example 1.

图4中,1为临界点,2为应力增量,3是应力增量为零的直线。In Figure 4, 1 is the critical point, 2 is the stress increment, and 3 is the straight line where the stress increment is zero.

图5是实施例2中直角坐标系下实验钢在950℃变形过程中的应力应变曲线。Figure 5 is the stress-strain curve of the experimental steel during deformation at 950°C in the Cartesian coordinate system in Example 2.

图6是实施例2中lgσ-lgε双对数坐标系下实验钢在950℃变形过程中的应力应变曲线。Figure 6 is the stress-strain curve of the experimental steel during deformation at 950°C in the lgσ-lgε double logarithmic coordinate system in Example 2.

图7是实施例2中实验钢在950℃变形应力应变曲线计算值与实验值对比图。Figure 7 is a comparison chart between the calculated values and experimental values of the deformation stress strain curve of the experimental steel at 950°C in Example 2.

图7中,1为应力应变曲线计算值,2为应力应变曲线实验值。In Figure 7, 1 is the calculated value of the stress-strain curve, and 2 is the experimental value of the stress-strain curve.

图8是实施例2中实验钢在950℃变形发生动态再结晶临界应变的确定示意图。Figure 8 is a schematic diagram for determining the critical strain of dynamic recrystallization of the experimental steel deformed at 950°C in Example 2.

图8中,1为临界点,2为应力增量,3是应力增量为零的直线。In Figure 8, 1 is the critical point, 2 is the stress increment, and 3 is the straight line where the stress increment is zero.

具体实施方式Detailed ways

本发明所述一种确定材料发生动态再结晶临界条件的方法,包括如下步骤:The method of determining critical conditions for dynamic recrystallization of materials according to the present invention includes the following steps:

1)通过热力模拟实验对实验材料进行单道次压缩实验,得到实验材料变形过程中的应力应变曲线;对得到的应力应变曲线进行平滑处理,去除噪声对实验曲线的影响;1) Conduct a single-pass compression experiment on the experimental material through a thermal simulation experiment to obtain the stress-strain curve during the deformation process of the experimental material; smooth the obtained stress-strain curve to remove the influence of noise on the experimental curve;

2)将与步骤1)中所述应力应变曲线相对应的应力σ和应变ε数据取绝对值,即应力σ和应变ε均为正值;然后在σ-lgε半对数坐标系或在lgσ-lgε双对数坐标系内重新绘制应力应变曲线;2) Take the absolute value of the stress σ and strain ε data corresponding to the stress strain curve described in step 1), that is, the stress σ and strain ε are both positive values; then in the σ-lgε semi-logarithmic coordinate system or in lgσ -Redraw the stress-strain curve in the lgε logarithmic coordinate system;

3)根据步骤2)重新绘制的应力应变曲线的形状特征,标定线性段部分区间,在其中选择不同的子区间进行多次线性回归;选择回归系数R≥0.99的子区间获得的线性回归方程,回归方程用如下公式表示:3) According to the shape characteristics of the stress-strain curve redrawn in step 2), calibrate some intervals of the linear segment, and select different sub-intervals to perform multiple linear regressions; select the linear regression equation obtained from the sub-interval with a regression coefficient R≥0.99, The regression equation is expressed by the following formula:

σ1=A+Blgε (1)σ 1 =A+Blgε (1)

loσ2=A1+B1lgε (2)loσ 2 =A 1 +B 1 lgε (2)

式中,σ1为应力值;loσ2为应力值对数;A、B、A1、B1为回归系数;In the formula, σ 1 is the stress value; loσ 2 is the logarithm of the stress value; A, B, A 1 and B 1 are regression coefficients;

若子区间在σ-lgε半对数坐标系下选取,则选用公式(1),若子区间在lgσ-lgε双对数坐标系下选取,则选用公式(2);If the subinterval is selected under the σ-lgε semi-logarithmic coordinate system, then formula (1) is used; if the subinterval is selected under the lgσ-lgε double logarithmic coordinate system, then formula (2) is used;

4)以步骤2)中所述应变ε为自变量,采用步骤3)所述公式(1)或公式(2)计算应力值σ1或应力值对数lgσ2,将所计算的应力值或应力值对数与步骤2)所述应力σ或lgσ进行比较,得到如下公式:4) Using the strain ε described in step 2) as the independent variable, use the formula (1) or formula (2) described in step 3) to calculate the stress value σ 1 or the logarithm of the stress value lgσ 2 , and calculate the stress value or Compare the logarithm of the stress value with the stress σ or lgσ described in step 2) to obtain the following formula:

ξ1=σ1-σ (3)ξ 11 -σ (3)

ξ2=lgσ2-lgσ (4)ξ 2 =lgσ 2 -lgσ (4)

式中,ξ1为在σ-lgε半对数坐标系下的特征应力差,ξ2为在lgσ-lgε双对数坐标系下由于特征应力差异导致的增量;In the formula, ξ 1 is the characteristic stress difference under the σ-lgε semi-logarithmic coordinate system, ξ 2 is the increment caused by the characteristic stress difference under the lgσ-lgε double logarithmic coordinate system;

若子区间在σ-lgε半对数坐标系下选取,则选用公式(3)计算出ξ1,并在直角坐标系下绘制ξ1-ε曲线;若子区间在lgσ-lgε双对数坐标系下选取,则选用公式(4)计算出ξ2,并在直角坐标系下绘制ξ2-ε曲线;If the subinterval is selected under the σ-lgε semi-logarithmic coordinate system, use formula (3) to calculate ξ 1 and draw the ξ 1 -ε curve under the rectangular coordinate system; if the subinterval is selected under the lgσ-lgε double logarithmic coordinate system If selected, use formula (4) to calculate ξ 2 and draw the ξ 2 -ε curve in the Cartesian coordinate system;

5)对步骤4)中获得的ξ1-ε曲线或ξ2-ε曲线进行分析,可知该曲线在选定的应变子区间内值为零;当应变超出所选应变子区间时,随着应变增大到某一个数值,计算值将大于实验值,该数值即为材料发生动态再结晶的临界应变值。5) Analyze the ξ 1 -ε curve or ξ 2 -ε curve obtained in step 4). It can be seen that the value of this curve is zero in the selected strain sub-interval; when the strain exceeds the selected strain sub-interval, as the When the strain increases to a certain value, the calculated value will be greater than the experimental value. This value is the critical strain value for dynamic recrystallization of the material.

本发明中,对步骤4)中获得的ξ1-ε曲线或ξ2-ε曲线进行分析,可知该曲线在选定的应变子区间内值为零,因为在该区间内,由公式(3)或公式(4)所得计算值与实验值具有高度一致性,因此两者之差为零。当应变超出所选应变子区间时,随着应变增大到某一个数值时,计算值将大于实验值。这是由于材料在变形过程中要经历加工硬化和回复软化以及动态再结晶软化等过程,而在初始阶段发生的是加工硬化和回复软化过程,应力随着应变的增大而迅速增大,但增幅逐渐减小,当发生动态再结晶时应力随着应变的变化规律势必要改变,这就会破坏原来的变化规律,而发生突变,这一突变对应于上述计算值与实验值开始出现偏差时的应变值,由此可以确定发生动态再结晶的临界应变。In the present invention, by analyzing the ξ 1 -ε curve or ξ 2 -ε curve obtained in step 4), it can be seen that the value of the curve is zero in the selected strain sub-interval, because in this interval, according to the formula (3 ) or formula (4) is highly consistent with the experimental value, so the difference between the two is zero. When the strain exceeds the selected strain sub-interval, the calculated value will be greater than the experimental value as the strain increases to a certain value. This is because the material undergoes processes such as work hardening, recovery softening, and dynamic recrystallization softening during the deformation process. What occurs in the initial stage is the process of work hardening and recovery softening. The stress increases rapidly with the increase in strain, but The increase gradually decreases. When dynamic recrystallization occurs, the change pattern of stress with strain is bound to change, which will destroy the original change pattern and cause a sudden change. This sudden change corresponds to when the above calculated values begin to deviate from the experimental values. strain value, from which the critical strain at which dynamic recrystallization occurs can be determined.

下面结合附图对本发明的具体实施方式作进一步说明:The specific embodiments of the present invention will be further described below in conjunction with the accompanying drawings:

以下实施例在以本发明技术方案为前提下进行实施,给出了详细的实施方式和具体的操作过程,但本发明的保护范围不限于下述的实施例。The following examples are implemented on the premise of the technical solution of the present invention and provide detailed implementation modes and specific operating processes. However, the protection scope of the present invention is not limited to the following examples.

【实施例1】[Example 1]

本实施例中,确定材料发生动态再结晶临界条件的过程如下:In this embodiment, the process of determining the critical conditions for dynamic recrystallization of materials is as follows:

1.试样材料选用一种含有镍铬钼合金元素的合金钢,试样尺寸为通过热力模拟试验机对试样进行单道次压缩实验,将试样加热至1200℃,并在该温度下保温3分钟,然后降温至变形温度1000℃,在该温度下以应变速率0.1s-1进行压缩变形,得到试样变形过程中的应力应变曲线,并对该曲线进行平滑处理,去除实验时噪声对曲线的影响,如图1所示;1. The sample material is an alloy steel containing nickel-chromium-molybdenum alloy elements. The sample size is A single-pass compression test was performed on the sample through a thermal simulation testing machine. The sample was heated to 1200°C and kept at this temperature for 3 minutes, and then cooled to the deformation temperature of 1000°C. At this temperature, the strain rate was 0.1s - 1. Perform compression deformation to obtain the stress-strain curve during the deformation process of the sample, and smooth the curve to remove the influence of noise on the curve during the experiment, as shown in Figure 1;

2.将与步骤1所述应力应变曲线相对应的应力σ和应变ε数据取绝对值,即将相应数值改为正值,然后在σ-lgε半对数坐标系内重新绘制应力应变曲线,如图2所示;2. Take the absolute values of the stress σ and strain ε data corresponding to the stress strain curve described in step 1, that is, change the corresponding values to positive values, and then redraw the stress strain curve in the σ-lgε semi-logarithmic coordinate system, such as As shown in Figure 2;

3.在图2中标定线性段部分区间,选择子区间(0.056,0.180)进行线性回归,得到的回归系数R=0.9996,回归方程为:3. Calibrate some intervals of the linear segment in Figure 2, select the sub-interval (0.056, 0.180) for linear regression, and obtain the regression coefficient R = 0.9996. The regression equation is:

σ1=147.228+52.544lgε (5)σ 1 =147.228+52.544lgε (5)

4.以步骤2所述应变为自变量,采用公式(5)计算应力值σ1,将所计算的应力值与实验值相比较,并将实验值与计算值对应的曲线绘制于同一坐标系中,如图3所示;4. Use the strain described in step 2 as the independent variable, use formula (5) to calculate the stress value σ 1 , compare the calculated stress value with the experimental value, and draw the curve corresponding to the experimental value and the calculated value in the same coordinate system , as shown in Figure 3;

5.将图3中曲线的纵坐标应力值做差,获得ξ1-ε曲线,可知该曲线在选定的应变子区间内值为零,在坐标系内做ξ1=0直线,则在选定的应变子区间内,直线ξ1=0与曲线ξ1-ε重合,进一步增大应变,两曲线开始发生偏离,开始偏离点即确定为试样发生动态再结晶的临界点,此时的应变确定为试样发生动态再结晶的临界应变,如图4所示。5. Difference the ordinate stress values of the curve in Figure 3 to obtain the ξ 1 -ε curve. It can be seen that the value of this curve is zero in the selected strain sub-interval. Draw a ξ 1 = 0 straight line in the coordinate system, then in Within the selected strain sub-interval, the straight line ξ 1 =0 coincides with the curve ξ 1 -ε. As the strain further increases, the two curves begin to deviate. The starting point of deviation is determined as the critical point for dynamic recrystallization of the sample. At this time The strain is determined as the critical strain for dynamic recrystallization of the sample, as shown in Figure 4.

【实施例2】[Example 2]

本实施例中,确定材料发生动态再结晶临界条件的过程如下:In this embodiment, the process of determining the critical conditions for dynamic recrystallization of materials is as follows:

1.试样材料选用一种低碳微合金钢,试样尺寸为通过热力模拟试验机对试样进行单道次压缩实验,将试样加热至1200℃,并在该温度下保温3分钟,然后降温至变形温度950℃,在该温度下以应变速率0.1s-1进行压缩变形,得到试样变形过程中的应力应变曲线,并对曲线进行平滑处理,去除实验时噪声对曲线的影响,如图5所示;1. The sample material is a low carbon microalloy steel, and the sample size is A single-pass compression test was performed on the sample through a thermal simulation testing machine. The sample was heated to 1200°C and kept at this temperature for 3 minutes, and then cooled to the deformation temperature of 950°C. At this temperature, the strain rate was 0.1s - 1. Perform compression deformation to obtain the stress-strain curve during the deformation process of the sample, and smooth the curve to remove the influence of noise on the curve during the experiment, as shown in Figure 5;

2.将与步骤1所述应力应变曲线相对应的应力σ和应变ε数据取绝对值,即将相应数值改为正值,然后在lgσ-lgε双对数坐标系内重新绘制应力应变曲线,如图6所示;2. Take the absolute values of the stress σ and strain ε data corresponding to the stress strain curve described in step 1, that is, change the corresponding values to positive values, and then redraw the stress strain curve in the lgσ-lgε double logarithmic coordinate system, such as As shown in Figure 6;

3.在图6中标定线性段部分区间,选择子区间(0.030,0.110)进行线性回归,得到的回归系数R=0.9993,回归方程为:3. Calibrate some intervals of the linear segment in Figure 6, select the sub-interval (0.030, 0.110) for linear regression, and obtain the regression coefficient R = 0.9993. The regression equation is:

lgσ2=2.12244+0.1252lgε (6)lgσ 2 =2.12244+0.1252lgε (6)

4.以步骤2所述应变为自变量,采用公式(6)计算应力值σ2,将所计算的应力值与实验值相比较,并将实验值与计算值对应的曲线绘制于同一坐标系中,如图7所示;4. Use the strain described in step 2 as the independent variable, use formula (6) to calculate the stress value σ 2 , compare the calculated stress value with the experimental value, and draw the curve corresponding to the experimental value and the calculated value in the same coordinate system , as shown in Figure 7;

5.将图7中曲线的纵坐标应力值做差,获得ξ2-ε曲线,可知该曲线在选定的应变子区间内值为零,在坐标系内做ξ2=0直线,则在选定的应变子区间内,直线ξ2=0与曲线ξ2-ε重合,进一步增大应变,两曲线开始发生偏离,开始偏离点即确定为发生动态再结晶的临界点,此时的应变确定为发生动态再结晶的临界应变,如图8所示。5. Difference the ordinate stress values of the curve in Figure 7 to obtain the ξ 2 -ε curve. It can be seen that the value of this curve is zero in the selected strain sub-interval. Draw a ξ 2 =0 straight line in the coordinate system, then in Within the selected strain sub-interval, the straight line ξ 2 =0 coincides with the curve ξ 2 -ε. As the strain further increases, the two curves begin to deviate. The starting point of deviation is determined as the critical point for dynamic recrystallization. The strain at this time The critical strain at which dynamic recrystallization occurs is determined, as shown in Figure 8.

以上所述,仅为本发明较佳的具体实施方式,但本发明的保护范围并不局限于此,任何熟悉本技术领域的技术人员在本发明揭露的技术范围内,根据本发明的技术方案及其发明构思加以等同替换或改变,都应涵盖在本发明的保护范围之内。The above are only preferred specific embodiments of the present invention, but the protection scope of the present invention is not limited thereto. Any person familiar with the technical field can, within the technical scope disclosed in the present invention, implement the technical solutions of the present invention. Equivalent substitutions or changes of the inventive concept thereof shall be included in the protection scope of the present invention.

Claims (1)

1.一种确定材料发生动态再结晶临界条件的方法,其特征在于,包括如下步骤:1. A method for determining critical conditions for dynamic recrystallization of materials, characterized by comprising the following steps: 1)通过热力模拟实验对实验材料进行单道次压缩实验,得到实验材料变形过程中的应力应变曲线;对得到的应力应变曲线进行平滑处理,去除噪声对实验曲线的影响;1) Conduct a single-pass compression experiment on the experimental material through a thermal simulation experiment to obtain the stress-strain curve during the deformation process of the experimental material; smooth the obtained stress-strain curve to remove the influence of noise on the experimental curve; 2)将与步骤1)中所述应力应变曲线相对应的应力σ和应变ε数据取绝对值,即应力σ和应变ε均为正值;然后在σ-lgε半对数坐标系或在lgσ-lgε双对数坐标系内重新绘制应力应变曲线;2) Take the absolute value of the stress σ and strain ε data corresponding to the stress strain curve described in step 1), that is, the stress σ and strain ε are both positive values; then in the σ-lgε semi-logarithmic coordinate system or in lgσ -Redraw the stress-strain curve in the lgε logarithmic coordinate system; 3)根据步骤2)重新绘制的应力应变曲线的形状特征,标定线性段部分区间,在其中选择不同的子区间进行多次线性回归;选择回归系数R≥0.99的子区间获得的线性回归方程,回归方程用如下公式表示:3) According to the shape characteristics of the stress-strain curve redrawn in step 2), calibrate some intervals of the linear segment, and select different sub-intervals to perform multiple linear regressions; select the linear regression equation obtained from the sub-interval with a regression coefficient R≥0.99, The regression equation is expressed by the following formula: σ1=A+Blgε (1)σ 1 =A+Blgε (1) lgσ2=A1+B1lgε (2)lgσ 2 =A 1 +B 1 lgε (2) 式中,σ1为应力值;lgσ2为应力值对数;A、B、A1、B1为回归系数;In the formula, σ 1 is the stress value; lgσ 2 is the logarithm of the stress value; A, B, A 1 and B 1 are regression coefficients; 若子区间在σ-lgε半对数坐标系下选取,则选用公式(1),若子区间在lgσ-lgε双对数坐标系下选取,则选用公式(2);If the subinterval is selected under the σ-lgε semi-logarithmic coordinate system, then formula (1) is used; if the subinterval is selected under the lgσ-lgε double logarithmic coordinate system, then formula (2) is used; 4)以步骤2)中所述应变ε为自变量,采用步骤3)所述公式(1)或公式(2)计算应力值σ1或应力值对数lgσ2,将所计算的应力值或应力值对数与步骤2)所述应力σ或lgσ进行比较,得到如下公式:4) Using the strain ε described in step 2) as the independent variable, use the formula (1) or formula (2) described in step 3) to calculate the stress value σ 1 or the logarithm of the stress value lgσ 2 , and calculate the stress value or Compare the logarithm of the stress value with the stress σ or lgσ described in step 2) to obtain the following formula: ξ1=σ1-σ (3)ξ 11 -σ (3) ξ2=lgσ2-lgσ (4)ξ 2 =lgσ 2 -lgσ (4) 式中,ξ1为在σ-lgε半对数坐标系下的特征应力差,ξ2为在lgσ-lgε双对数坐标系下由于特征应力差异导致的增量;In the formula, ξ 1 is the characteristic stress difference under the σ-lgε semi-logarithmic coordinate system, ξ 2 is the increment caused by the characteristic stress difference under the lgσ-lgε double logarithmic coordinate system; 若子区间在σ-lgε半对数坐标系下选取,则选用公式(3)计算出ξ1,并在直角坐标系下绘制ξ1-ε曲线;若子区间在lgσ-lgε双对数坐标系下选取,则选用公式(4)计算出ξ2,并在直角坐标系下绘制ξ2-ε曲线;If the subinterval is selected under the σ-lgε semi-logarithmic coordinate system, use formula (3) to calculate ξ 1 and draw the ξ 1 -ε curve under the rectangular coordinate system; if the subinterval is selected under the lgσ-lgε double logarithmic coordinate system If selected, use formula (4) to calculate ξ 2 and draw the ξ 2 -ε curve in the Cartesian coordinate system; 5)对步骤4)中获得的ξ1-ε曲线或ξ2-ε曲线进行分析,可知该曲线在选定的应变子区间内值为零;当应变超出所选应变子区间时,随着应变增大到某一个数值,计算值将大于实验值,该数值即为材料发生动态再结晶的临界应变值。5) Analyze the ξ 1 -ε curve or ξ 2 -ε curve obtained in step 4). It can be seen that the value of this curve is zero in the selected strain sub-interval; when the strain exceeds the selected strain sub-interval, as the When the strain increases to a certain value, the calculated value will be greater than the experimental value. This value is the critical strain value for dynamic recrystallization of the material.
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Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102519801A (en) * 2011-12-16 2012-06-27 南京航空航天大学 Method for establishing aluminium alloy dynamic recrystallization model by using true stress-true strain curve
WO2014150342A1 (en) * 2013-03-15 2014-09-25 United Technologies Corporation Cast component having corner radius to reduce recrystallization
CN109255175A (en) * 2018-08-31 2019-01-22 西北工业大学 A kind of recrystallization control method based on critical recrystallization residual stress
CN109444039A (en) * 2018-09-21 2019-03-08 首钢集团有限公司 The method for predicting that dynamic recrystallization critical reduction occurs when controlled hot rolling of micro-alloyed steel
CN110702727A (en) * 2019-09-30 2020-01-17 鞍钢股份有限公司 A method for determining the static recrystallization volume fraction of materials
CN110849801A (en) * 2019-11-29 2020-02-28 西北有色金属研究院 Method for determining critical stress of metal low-speed deformation recrystallization
CN111933221A (en) * 2020-08-03 2020-11-13 东北大学 Method for predicting dynamic recrystallization fraction of Nb microalloyed steel

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102519801A (en) * 2011-12-16 2012-06-27 南京航空航天大学 Method for establishing aluminium alloy dynamic recrystallization model by using true stress-true strain curve
WO2014150342A1 (en) * 2013-03-15 2014-09-25 United Technologies Corporation Cast component having corner radius to reduce recrystallization
CN109255175A (en) * 2018-08-31 2019-01-22 西北工业大学 A kind of recrystallization control method based on critical recrystallization residual stress
CN109444039A (en) * 2018-09-21 2019-03-08 首钢集团有限公司 The method for predicting that dynamic recrystallization critical reduction occurs when controlled hot rolling of micro-alloyed steel
CN110702727A (en) * 2019-09-30 2020-01-17 鞍钢股份有限公司 A method for determining the static recrystallization volume fraction of materials
CN110849801A (en) * 2019-11-29 2020-02-28 西北有色金属研究院 Method for determining critical stress of metal low-speed deformation recrystallization
CN111933221A (en) * 2020-08-03 2020-11-13 东北大学 Method for predicting dynamic recrystallization fraction of Nb microalloyed steel

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