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We all remember the equation, {F} = [K] {u}, where F is the nodal force vector, K is the stiffness matrix and u is the nodal displacement vector. Well in a typical (linear) FEA model, this stiffness matrix, K, is defined at the beginning and it is assumed not to change throughout the entire analysis.


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The following approach will be used: 1. Look at force equilibrium of the element - assume that the sum of the nodal internal forces acting on the element is equal to zero. 2. Apply Hooke's law, which states that the stress \sigma σ is a linear function of the strain \epsilon ϵ. \begin {equation} \sigma = E \epsilon \end {equation} σ = E ϵ.


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where {F} is the applied force vector, {R} is the external reaction vector, [K] is the global stiffness matrix, and {U} is the nodal displacement vector.. In the equation above, {R} and {U} are unknowns. To simplify the solution of this equation, it is desired to solve for the reactions and displacements independently of one another.


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U = J [M][L] 2 [T] −2. , where F is not proportional to N because μ i depends on. = ⁡, where k B is the Boltzmann constant, and Ω denotes the volume of macrostate in the phase space or otherwise called thermodynamic probability. = , for reversible processes only; Statistical.


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Method of Finite Elements I Chapter 2 The Direct Stiffness Method Direct Stiffness Method (DSM) Computational method for structural analysis Matrix method for computing the member forces and displacements in structures DSM implementation is the basis of most commercial and open-source finite element software