Anh Tay Nguyen, Houlin Xu, Karel Matous, Zdenek P. Bazant
{"title":"基于应力-扭伤关系和位移梯度拉格朗日乘子约束的光滑拉格朗日裂纹带模型(slCBM","authors":"Anh Tay Nguyen, Houlin Xu, Karel Matous, Zdenek P. Bazant","doi":"10.1115/1.4063896","DOIUrl":null,"url":null,"abstract":"Abstract A preceding 2023 study argued that the resistance of a heterogeneous material to the displacement field curvature is the physically most realistic localization limiter for softening damage. The curvature was characterized by the second gradient of the displacement vector field, which includes the material rotation gradient, and was named the ‘sprain’ tensor, while the term ‘spress’ is here proposed as the force variable work-conjugate to ‘sprain’. In this study, the computational obstacles using nodal sprain forces in the previous study are overcome by using finite elements with linear shape functions for both the displacement vector and for an approximate displacement gradient tensor. The actual gradient calculated from the nodal displacement vectors is constrained to the approximate gradient by means of a Lagrange multiplier tensor. The gradient tensor of the approximate gradient tensor then represents the third-order approximate displacement curvature tensor (or Hessian) of the displacement field. Importantly, the Lagrange multiplier behaves as an externally applied generalized moment density that, similar to gravity, does not affect the total strain-plus-sprain energy density of material. The conditions of stationary values of the total free energy of the structure with respect all these unknowns yields the set of equilibrium equations of the structure for each loading step. Examples of crack growth in fracture specimens are given. It is demonstrated that the simulation results are independent of the orientation of a regular square mesh, and capture the width variation of the crack band, and converge as the finite elements are refined.","PeriodicalId":54880,"journal":{"name":"Journal of Applied Mechanics-Transactions of the Asme","volume":"67 1","pages":"0"},"PeriodicalIF":2.6000,"publicationDate":"2023-10-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Smooth Lagrangian Crack Band Model (slCBM) Based on Spress-Sprain Relation and Lagrange Multiplier Constraint of Displacement Gradient\",\"authors\":\"Anh Tay Nguyen, Houlin Xu, Karel Matous, Zdenek P. Bazant\",\"doi\":\"10.1115/1.4063896\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Abstract A preceding 2023 study argued that the resistance of a heterogeneous material to the displacement field curvature is the physically most realistic localization limiter for softening damage. The curvature was characterized by the second gradient of the displacement vector field, which includes the material rotation gradient, and was named the ‘sprain’ tensor, while the term ‘spress’ is here proposed as the force variable work-conjugate to ‘sprain’. In this study, the computational obstacles using nodal sprain forces in the previous study are overcome by using finite elements with linear shape functions for both the displacement vector and for an approximate displacement gradient tensor. The actual gradient calculated from the nodal displacement vectors is constrained to the approximate gradient by means of a Lagrange multiplier tensor. The gradient tensor of the approximate gradient tensor then represents the third-order approximate displacement curvature tensor (or Hessian) of the displacement field. Importantly, the Lagrange multiplier behaves as an externally applied generalized moment density that, similar to gravity, does not affect the total strain-plus-sprain energy density of material. The conditions of stationary values of the total free energy of the structure with respect all these unknowns yields the set of equilibrium equations of the structure for each loading step. Examples of crack growth in fracture specimens are given. It is demonstrated that the simulation results are independent of the orientation of a regular square mesh, and capture the width variation of the crack band, and converge as the finite elements are refined.\",\"PeriodicalId\":54880,\"journal\":{\"name\":\"Journal of Applied Mechanics-Transactions of the Asme\",\"volume\":\"67 1\",\"pages\":\"0\"},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2023-10-26\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Applied Mechanics-Transactions of the Asme\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1115/1.4063896\",\"RegionNum\":4,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MECHANICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Applied Mechanics-Transactions of the Asme","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1115/1.4063896","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MECHANICS","Score":null,"Total":0}
Smooth Lagrangian Crack Band Model (slCBM) Based on Spress-Sprain Relation and Lagrange Multiplier Constraint of Displacement Gradient
Abstract A preceding 2023 study argued that the resistance of a heterogeneous material to the displacement field curvature is the physically most realistic localization limiter for softening damage. The curvature was characterized by the second gradient of the displacement vector field, which includes the material rotation gradient, and was named the ‘sprain’ tensor, while the term ‘spress’ is here proposed as the force variable work-conjugate to ‘sprain’. In this study, the computational obstacles using nodal sprain forces in the previous study are overcome by using finite elements with linear shape functions for both the displacement vector and for an approximate displacement gradient tensor. The actual gradient calculated from the nodal displacement vectors is constrained to the approximate gradient by means of a Lagrange multiplier tensor. The gradient tensor of the approximate gradient tensor then represents the third-order approximate displacement curvature tensor (or Hessian) of the displacement field. Importantly, the Lagrange multiplier behaves as an externally applied generalized moment density that, similar to gravity, does not affect the total strain-plus-sprain energy density of material. The conditions of stationary values of the total free energy of the structure with respect all these unknowns yields the set of equilibrium equations of the structure for each loading step. Examples of crack growth in fracture specimens are given. It is demonstrated that the simulation results are independent of the orientation of a regular square mesh, and capture the width variation of the crack band, and converge as the finite elements are refined.
期刊介绍:
All areas of theoretical and applied mechanics including, but not limited to: Aerodynamics; Aeroelasticity; Biomechanics; Boundary layers; Composite materials; Computational mechanics; Constitutive modeling of materials; Dynamics; Elasticity; Experimental mechanics; Flow and fracture; Heat transport in fluid flows; Hydraulics; Impact; Internal flow; Mechanical properties of materials; Mechanics of shocks; Micromechanics; Nanomechanics; Plasticity; Stress analysis; Structures; Thermodynamics of materials and in flowing fluids; Thermo-mechanics; Turbulence; Vibration; Wave propagation