{"title":"软质复合柱崩塌的毛细控制","authors":"Marc Suñé, J. Wettlaufer","doi":"10.1103/PhysRevMaterials.5.055603","DOIUrl":null,"url":null,"abstract":"Euler buckling is the elastic instability of a column subjected to longitudinal compressing forces at its ends. The buckling instability occurs when the compressing load reaches a critical value and an infinitesimal deflection leads to a large amplitude deflection. Since Euler's original study, this process has been extensively studied in homogeneous, isotropic, linear-elastic solids. Here, we examine the nature of the buckling in inhomogeneous soft composite materials. In particular, we consider a soft host with liquid inclusions both large and small relative to the elastocapillarity length, which lead to softening and stiffening of a homogeneous composite respectively. However, by imposing a gradient of the volume fraction or varying the inclusion size we can deliberately manipulate the nature of Euler buckling.","PeriodicalId":8472,"journal":{"name":"arXiv: Soft Condensed Matter","volume":"40 12 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2020-05-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Capillary control of collapse in soft composite columns\",\"authors\":\"Marc Suñé, J. Wettlaufer\",\"doi\":\"10.1103/PhysRevMaterials.5.055603\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Euler buckling is the elastic instability of a column subjected to longitudinal compressing forces at its ends. The buckling instability occurs when the compressing load reaches a critical value and an infinitesimal deflection leads to a large amplitude deflection. Since Euler's original study, this process has been extensively studied in homogeneous, isotropic, linear-elastic solids. Here, we examine the nature of the buckling in inhomogeneous soft composite materials. In particular, we consider a soft host with liquid inclusions both large and small relative to the elastocapillarity length, which lead to softening and stiffening of a homogeneous composite respectively. However, by imposing a gradient of the volume fraction or varying the inclusion size we can deliberately manipulate the nature of Euler buckling.\",\"PeriodicalId\":8472,\"journal\":{\"name\":\"arXiv: Soft Condensed Matter\",\"volume\":\"40 12 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2020-05-19\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv: Soft Condensed Matter\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1103/PhysRevMaterials.5.055603\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv: Soft Condensed Matter","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1103/PhysRevMaterials.5.055603","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Capillary control of collapse in soft composite columns
Euler buckling is the elastic instability of a column subjected to longitudinal compressing forces at its ends. The buckling instability occurs when the compressing load reaches a critical value and an infinitesimal deflection leads to a large amplitude deflection. Since Euler's original study, this process has been extensively studied in homogeneous, isotropic, linear-elastic solids. Here, we examine the nature of the buckling in inhomogeneous soft composite materials. In particular, we consider a soft host with liquid inclusions both large and small relative to the elastocapillarity length, which lead to softening and stiffening of a homogeneous composite respectively. However, by imposing a gradient of the volume fraction or varying the inclusion size we can deliberately manipulate the nature of Euler buckling.