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1 Answer Sorted by: 1 Adapted from this lecture notes page 9. The approach splits the matrix and right-hand side into Dirichlet and free nodes: K = ( K D D K D f K f D K f f) F = ( F D F f) In your case the free nodes have the indices { 6, 7, 8 } .


K U F I C .2 on Behance

The goal of modal analysis in structural mechanics is to determine the natural mode shapes and frequencies of an object or structure during free vibration.It is common to use the finite element method (FEM) to perform this analysis because, like other calculations using the FEM, the object being analyzed can have arbitrary shape and the results of the calculations are acceptable.


K U F I C .2 on Behance

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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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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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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