Yu. A. Belokon’, A. Yavtushenko, V. Protsenko, Y. Bondarenko, A. Cheilytko
{"title":"MATHEMATICAL MODELING OF PHYSICAL PROPERTIES OF ANISOTROPIC MATERIALS","authors":"Yu. A. Belokon’, A. Yavtushenko, V. Protsenko, Y. Bondarenko, A. Cheilytko","doi":"10.37904/metal.2020.3500","DOIUrl":null,"url":null,"abstract":"The problem of selecting a material with an extreme value of its performance using its anisotropy is considered. It is important for specialists of metallurgical profile to be able not only to select the material for realization of the set engineering task, but also to use its anisotropy, and to be able to determine the orientation of the material with the extreme value of its performance. Mathematical modeling and computer analysis of anisotropy of tensor coefficients using the example of thermal expansion coefficient have been performed. Since thermal expansion, like any tensor physical property of crystals, is a continuous function of direction, then in order to determine the directions with a zero value of thermal expansion, the following ratio must be satisfied: αn = 0. This can only happen if the main components of the thermal expansion tensor have different symbols. The Mathcad Prime 6 software complex has defined a function that performs the calculation of the value of thermal expansion coefficients in crystals in any direction, calculated the value and position of extremums of thermal expansion coefficients, and constructed an index surface, a stereographic projection of the index surface and the cross section of the index surface of thermal expansion coefficients X1X3. The lowest and highest values of the thermal expansion coefficient of the crystal have been found.","PeriodicalId":21337,"journal":{"name":"Revue De Metallurgie-cahiers D Informations Techniques","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2020-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Revue De Metallurgie-cahiers D Informations Techniques","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.37904/metal.2020.3500","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The problem of selecting a material with an extreme value of its performance using its anisotropy is considered. It is important for specialists of metallurgical profile to be able not only to select the material for realization of the set engineering task, but also to use its anisotropy, and to be able to determine the orientation of the material with the extreme value of its performance. Mathematical modeling and computer analysis of anisotropy of tensor coefficients using the example of thermal expansion coefficient have been performed. Since thermal expansion, like any tensor physical property of crystals, is a continuous function of direction, then in order to determine the directions with a zero value of thermal expansion, the following ratio must be satisfied: αn = 0. This can only happen if the main components of the thermal expansion tensor have different symbols. The Mathcad Prime 6 software complex has defined a function that performs the calculation of the value of thermal expansion coefficients in crystals in any direction, calculated the value and position of extremums of thermal expansion coefficients, and constructed an index surface, a stereographic projection of the index surface and the cross section of the index surface of thermal expansion coefficients X1X3. The lowest and highest values of the thermal expansion coefficient of the crystal have been found.
考虑了利用材料的各向异性选择具有极值性能的材料的问题。对于冶金型材专家来说,不仅要能够为完成既定的工程任务而选择材料,而且要能够利用材料的各向异性,并能够利用材料性能的极值来确定材料的取向。以热膨胀系数为例,对张量系数的各向异性进行了数学建模和计算机分析。由于热膨胀与晶体的任何张量物理性质一样,是方向的连续函数,因此为了确定热膨胀为零的方向,必须满足以下比值:αn = 0。只有当热膨胀张量的主要分量有不同的符号时,这种情况才会发生。Mathcad Prime 6软件复合体定义了计算晶体任意方向热膨胀系数值的函数,计算了热膨胀系数极值的值和位置,构造了一个指标面、指标面的立体投影和热膨胀系数X1X3的指标面截面。得到了晶体热膨胀系数的最小值和最大值。