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The displacement field u, which has two components (u, v) in 2D and three components (u, v, and w) in 3D.
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The rotation angle θ, which has one component in 2D (th) and three components in 3D (thx, thy, and thz).
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The dependent variable names remain same in both a geometrically linear and a geometrically nonlinear analysis. Under geometric nonlinearity, the dependent variables are however not defined though shape functions. The equivalent shape function variables are (beam.uLinx, beam.uLiny, beam.uLinz) and (beam.thLinx, beam.thLiny, beam.thLinz). In this case, you will see the latter names under Dependent Variables in the Solver Configurations tree.
If needed, these shape variables can be used to write any extra contributions in the Beam interface.
If a physics interface that separates the material and spatial frame (Solid Mechanics is one such example) is added to the model, the coordinate indices change from (x, y, z) to (X, Y, Z) in the name of these variables.
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