G+Smo  23.12.0
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Linear buckling analysis is performed by solving the following eigenvalue problem:

\[ (K_L-\sigma K_{NL}(\mathbf{u}^L_h))\mathbf{v}_h = \lambda K_{NL}(\mathbf{u}_h) \mathbf{v}_h \]

Where \(K_L\) is the linear stiffness matrix, \(K_{NL}(\mathbf{u}_h)\) is the tangential stiffness matrix assembled around \(\mathbf{u}^L_h\). The solution \(\mathbf{u}^L_h\) is obtained by solving a linear problem \(K_L\mathbf{u}^L_h = \mathbf{P}\). Furthermore, \(\sigma\) is a shift and \((\lambda+\sigma\f)\mathbf{P}\) is the critical buckling load. The modeshape is represented by \(\phi\).

Examples with the use of this class are: