{"title":"On Generalizations of the Minimal Complementary Energy Variational Principle in Linear Elastostatics","authors":"Jiashi Yang","doi":"arxiv-2409.06875","DOIUrl":null,"url":null,"abstract":"It is shown that when the well-known minimal complementary energy variational\nprinciple in linear elastostatics is written in a different form with the\nstrain tensor as an independent variable and the constitutive relation as one\nof the constraints, the removal of the constraints by Lagrange multipliers\nleads to a three-field variational principle with the displacement vector,\nstress field and strain field as independent variables. This three-field\nvariational principle is without constrains and its variational functional is\ndifferent from those of the existing three-field variational principles. The\ngeneralization is not unique. The procedure is mathematical and may be used in\nother branches of physics.","PeriodicalId":501482,"journal":{"name":"arXiv - PHYS - Classical Physics","volume":"25 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Classical Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.06875","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
It is shown that when the well-known minimal complementary energy variational
principle in linear elastostatics is written in a different form with the
strain tensor as an independent variable and the constitutive relation as one
of the constraints, the removal of the constraints by Lagrange multipliers
leads to a three-field variational principle with the displacement vector,
stress field and strain field as independent variables. This three-field
variational principle is without constrains and its variational functional is
different from those of the existing three-field variational principles. The
generalization is not unique. The procedure is mathematical and may be used in
other branches of physics.