The fundamental concept of the finite element method is that a physical domain is discretised into a small number of sub-domains, known as elements, over which a continuous field variable such as velocity, stress, pressure, or temperature can be approximated. These elements are connected at specific points known as nodes or nodal points. Since the actual variation of the field variable is not known inside the domain, approximating functions are needed to describe this variation. These approximating
establishing formulation of Finite Element Method of a 2-Dimensional Kirchhoff Plate. This study investigate the behavior of plates based on Kirchhoff theory of thin plates in plane stress, the study established the formulation of the FEM to the plate in the previous chapter there for this chapter will show the results and discussion of the formulation by implying it on an actual case study to verify the accuracy of the formulation and the developed algorithm by two methods in FEM solution using analytical
[1]. However, the classical solution frequently no exists and for those problems where is possible the use of these analytical methods, many simplifications are done [2]. Consequently, several numerical methods have been developed to efficiently solve EPDE such as the finite element method (FEM), finite difference and others. The FEM have several advantages over other methods. The main advantage is that it is particularly effective for problems with complicated geometry using unstructured meshes [2]
larger than theoretical cohesive strength will generally cause local plastic deformation and redistribution of stresses [3].There are different ways of determining the stress concentration factor in flat plates. Experimental, numerical and analytical methods are used to determine stress
domains, the finite element method is a natural choice for many researchers (e.g. \cite{118}). However, in the context of singularly-perturbed convection-diffusion problems, it is difficult to construct monotone methods on highly anisotropic meshes, which are desirable when thin layers are present. Moreover, energy norms or other norms based on the $L^2-$norm, are the natural norms associated with variational methods. Error analysis in the pointwise norm is not straightforward in a finite element framework
associated with diffuse axonal injury over years. Diffusion tensor imaging (DTI) is one such technique where the mesoscale structural information is studied to investigate the diffuse axonal injury. Finite element models have also provided a means to investigate diffuse axonal injury. Several finite element head models have been developed and reported in the literature (citealt{shugar1977,ward1980,hosey1982,Ruan1991,mendis1992,bandak1995,kang1997,al1999,Zhang2001,Kleiven2002,brands2002,takhounts2003
list of finite element studies that included diffusion tensor imaging tractography in the injury analysis. Most of the studies (citealt{colgan2010, wright2012, wright2013, Kraft2012, sahoo2014, kleiven2014}) used a diffusion tensor imaging apprised anisotropic material models to represent brain tissue during the analysis. The axonal strains were then calculated using explicit post processing steps. These studies mapped multiple voxels from DTI data to a single element in the finite element model using
associated with diffuse axonal injury over the years. Diffusion tensor imaging (DTI) is one such technique where the mesoscale structural information is studied to investigate the diffuse axonal injury. Finite element models have also provided a means to investigate diffuse axonal injury. Several finite element head models have been developed and reported in the literature (citealt{shugar1977,ward1980,hosey1982,Ruan1991,mendis1992,bandak1995,kang1997,al1999,Zhang2001,Kleiven2002,brands2002,takhounts2003
Review Context Freeform surfaces prevail in contemporary architecture. Over the past two decades there has been a surge in the use of smooth, curved surfaces, which can be attributed to improvements in 3D modelling techniques and advances in finite element analysis. The complex geometries, examples of which can be seen in the Figure ? below, pose challenges in developing a feasible building envelope using conventional building materials such as steel and concrete. This has therefore created a need
Mapped meshes are made according to requirements as it gives user control over size and shape and deformation of the mesh in all regions The surface stress on the microcantilever surface can be calculated from the observed microcantilever deflection using Stoney’s equation Where Δσs is the differential surface stresses on the surface of the microcantilever, is the Young’s modulus, is the Poisson’s ratio r and h are the radius of curvature and thickness of cantilever beam respectively.For a two-layer