CUSTOMER SUPPORT NOTE Nonlinear Buckling Analysis with Initial Imperfection Note Number: CSN/LUSAS/1014 This support note is issued as a guideline only. © Finite Element Analysis Ltd. © Finite Element Analysis Ltd 2011 CSN/LUSAS/1014 Table of Contents 1. INTRODUCTION 1 2. DESCRIPTION 2 CSN/LUSAS/1014 1. Introduction In a nonlinear buckling analysis, a small perturbation load could be applied to encourage convergence past buckling and onto a post-buckling path. This load should be small enough such that it does not affect the results, but just disturbs the symmetry of the mesh enough to encourage a particular post-buckling path. An alternative method for a post-buckling solution is to use slightly deformed initial mesh or geometry. This may be achieved when defining the geometry, or by using a deformed mesh from a separate analysis. For example the deformed mesh of an eigen value buckling analysis may be used as a starting point for the mesh in a subsequent and separate nonlinear buckling analysis. This latter option may well be convenient if an eigenvalue buckling or a frequency analysis has already been performed on the same model. Page 1 CSN/LUSAS/1014 © Finite Element Analysis Ltd 2011 2. Description To achieve a post-buckling solution, an initial deformed shape can be either created by actually building the model with an imperfection in the geometry or by using the deformed shape from another analysis (say from eigenvalue, static or linear eigenvalue buckling analysis). A linear (eigenvalue) buckling analysis will produce critical buckling loads and buckled shapes. The results of this analysis are normalised displacements due to eigenvector unity normalisation. A factored deformed shape from this linear buckling analysis can then be used as the initial mesh for a further nonlinear buckling analysis to develop post-buckling behaviour. Load Initial imperfect geometry Critical buckling load Development of post-buckled shape under NL incremental loading Incremental nonlinear buckling analysis Linear Buckling Analysis Non-linear Analysis Formulate model as linear problem with perfect geometry Solve eigenproblem for critical loads and buckled configurations If required, ‘tabulate’ reduced deformed shape as imperfect initial geometry for non-linear analysis Formulate GNL analysis based on initially imperfect geometry Increment loading and progressively develop true post-buckled configuration For example, an eigenvalue buckling analysis of the plate girder has been run and the buckling load has been calculated for the girder. In figure 1 the deformed shape of the girder Page 2 CSN/LUSAS/1014 © Finite Element Analysis Ltd 2011 is shown. When an eigenvalue buckling analysis is performed the displacements are unity normalised, in this case as the model has been built in metres unity being one metre. Figure 1 To use the deformed mesh of such an analysis follow the steps below. 1. Create a new model for a subsequent nonlinear buckling analysis. It is suggested to save a copy of the model used for the eigenvalue buckling analysis (or any other acceptable model) with a different name. This will ensure that the mesh used is that same in both models (an essential condition of using an initial deformed mesh). This model can then be set up to perform a nonlinear analysis with geometric nonlinearity. 2. In this new model, to specify a nonlinear solution, you must add a Nonlinear and Transient Control to the Loadcase (right-click on the loadcase>Controls>Nonlinear and Transient) in place of the Eigenvalue control. 3. The inclusion of Geometric Nonlinearity (GNL) is required in a nonlinear buckling analysis. For a Nonlinear Buckling Analysis, elements that have a geometric nonlinearity formulation must therefore be used. The geometric nonlinearity formulations supported by the elements being used can be checked in the Element Reference Manual. The chosen suitable formulation to be used is then set in the Nonlinear Options in the Loadcase TreeView (or via File>Model Properties>Solution tab>Nonlinear Options). If different elements are used with different formulations for GNL, more than one option can be selected in the Nonlinear Options. 4. Once the model is ready to analyse, the results file of the first model (eigenvalue buckling analysis in this example) can be opened on top of the current, nonlinear model. To now use the deformed shape from the initial analysis the required results from the required loadcase must first be set active (see Figure 2). Page 3 CSN/LUSAS/1014 © Finite Element Analysis Ltd 2011 Figure 2 5. Then go to Utilities>Mesh>Use Deformations… menu option, as shown in Figure 3. Enter a scaling factor that is required. In this case by entering the value of 0.015 it will scale the one metre deflection down to 15mm. ( 1 x 0.015 = 0.015m = 15 mm). Note that for a nonlinear buckling analysis where you are using an initial imperfection, that the minimal imperfection required should be used; just enough to encourage convergence past buckling and onto a post-buckling path. Figure 3 6. Once the scaling factor has been entered click OK and then solve the new nonlinear buckling analysis. This method adjusts the coordinates of all nodes in the mesh to include the imperfection using the supplied deformed mesh factor. It is important to note that the deformed mesh will be saved in the model until the mesh is reset (Utilities>Mesh>Mesh Reset), even if the model is closed and reopened. Please see the Modeller Reference Manual>Chapter 7 : Running an Analysis>LUSAS Analyses Types>Nonlinear Analysis and the guidance in the user area of our website for further information. Page 4
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