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Interactions finite strain

These observations are equivalent to a coarse-grained view of the system, which is tantamount to a description in terms of continuum mechanics. [It is clear that "points" of the continuum may not refer to such small collections of atoms that thermal fluctuations of the coordinates of their centers of mass become substantial fractions of their strain displacements.] The elastomer is thus considered to consist of a large number of quasi-finite elements, which interact with one another through dividing surfaces. [Pg.244]

This problem falls into a category of strongly coupled fluid-structure interaction (FSI) problems due to comparable stiffnesses of the container and its liquid content. Hence, accurate prediction of containers behaviour requires a liquid-container interaction model. Here, a two-system FSI model based on the Finite Volume Method is employed, and a good agreement is found between measured and predicted pressure and strain histories. [Pg.253]

This model is based on quasimolecular dynamics, in which the medium is assumed to be composed of an assembly of meso-scale discrete particles (i.e., finite elements). Tlie movement and deformation of the material system and its evolution are described by the aggregate movements of these elements. Two types of basic characteristics, geometrical and physical, are considered. In tlie geometrical aspect, sliapes and sizes of elements and tlie manner of their initial aggregation and arrangement are the important factors. In the physical aspect, mechanical, physical, and chemical characteristics, such as the interaction potential, phase transition, and chemical reactivity may be tlie important ones. To construct this model, many physical factors, including interaction potential, friction of particles, shear resistance force, energy dissipation and temperature increase, stress and strain at the meso- and macro-levels, phase transition, and chemical reaction are considered. In fact, simulation of chemical reactions is one of the most difficult tasks, but it is the most important aspect in shock-wave chemistiy. [Pg.216]

Sun, Z., Howard, D. and Moatamedi, M., 2005. Finite element analysis of footwear and ground interaction. Strain, 41(3), 113-15. [Pg.164]

Finite elements analysis has shown that filler properties such as surface area, shape and structure have strong infiuence on the filler reinforcement and filler rubber properties. Another approach to understand the filler network and the filler-rubber interactions more closely is to study the electrical and mechanical behaviour of the filled elastomer under strain for various different conditions. Jha et have investigated the effect of surface area and structure of filler... [Pg.112]

ABSTRACT In the present paper a multiphase model including a hypoplastic formulation of the solid phase is presented and its application to earthquake engineering problems discussed. The macroscopic soil model, which is based on the theory of porous media, comprises three distinct phases namely, solid, fluid and gas phase. For each of these the compressibility of the respective medium is taken into account in the mathematical formulation of the model. The solid phase is modelled using the hypoplastic constitutive equation including intergranular strain to allow for a realistic description of material behaviour of cohesionless soils even under cyclic loading. The model was implemented into the finite element package ANSYS via the user interface and also allows the simulation of soil-structure interaction problems. [Pg.293]

To overcome these problems, a multiphase model considering a hypoplastic approach including intergranular strain for the solid phase has been developed in this work. Due to its implementation into the finite element program ANSYS it also allows for soil-structure-interaction analyses within the existing finite element framework. In Holler Meskouris (2006), presented the application of the model to a soil-strncture interaction analysis of silos under dynamic excitation. [Pg.294]

Finite element modeling (FEM) can be invaluable in developing and/or applying acceleration models for thermal and mechanical tests. Two-dimensional nonlinear modeling capability will usually be required in order to get meaningful results. Models can be constructed to estimate the stresses and strains in the material (e.g., the Cu in a PTH barrel or the solder in a surface-mount or through-hole joint) under operating conditions as well as under test conditions. These estimates will be far more accurate than the simple models provided in this overview because they can account for the interactions between materials in a complex structure and both elastic and plastic deformation. [Pg.1354]

Andrianopoulos et al. (2006), Lopez-Caballero and Modaressi Farahmand-Razavi (2008), Andrianopoulos et al. (2010), Shahir and Pak (2010), Dashti and Bray (2013), Lopez-Caballero and Modaressi Farahmand-Razavi (2013), and Karamitros et al. (2013) conducted 2-D (plane strain) and 3-D, fully coupled, nonlinear, finite element and finite difference analyses to study the dynamic interaction between homogeneous and layered liquefiable sand and a structure. In these analyses, the stmcture was simulated either as a surface load, rigid stmcture, or an elastic SDOF model. The foundation was mostly... [Pg.1336]

Where a is the equivalent stress, (7y is the yield stress of the matrix material and akk is the hydrostatic stress. The parameters qi and q2 were introduced by Tvergaard to account for the effect of void interactions on the stress distribution between cavities, but are usually derived from finite element calibration of experimental curves. Damage evolution is measured by the void volume fraction f, which increases due to void nucleation and growth. Void nucleation is controlled by a normal distribution of stress or plastic strain and the modified model replaces the void volume fraction /with the modified void volume fraction /. A rapid decrease in the load carrying capacity of the material if void coalescence occurs is linked to /, such that... [Pg.818]


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Interaction strain

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