vibration of a displaced beam
We consider an analysis that combines both static and dynamic steps. A simple cantilever beam with point mass is displaced in the static step and released in the dynamic step.
The model can be dowloaded.
Model Definition
First, we define two nodes at and .
node 1 0 0
node 2 1 0To simply the example, we use elastic material and the EB21 element, so that there is no need to define beam sections. A point mass of magnitude of is applied to node DoF .
material Elastic1D 1 10
element EB21 1 1 2 12 1 1
element Mass 2 2 2 2Then we fix point .
fix 1 P 1We record the displacement of node as the result.
hdf5recorder 1 Node U2 2Static Step
For the static step, a displacement load is applied on node DoF . The absolute increment displacement is tested for convergence.
step static 1 1
set ini_step_size .1
displacement 1 0 1 2 2
converger AbsIncreDisp 1 1E-8 3 1Dynamic Step
A dynamic step with step size of can then be defined. There is no need to define any load in this step. The previous displacement load is by default active for only one step. Hence, in this dynamic step, the displacement load is automatically suspended. A default Newmark integrator will be automatically defined if there is no valid integrator.
step dynamic 2 2
set ini_step_size .02
set fixed_step_size 1
converger AbsIncreDisp 2 1E-8 3 1Run Analysis
analyze
save recorder 1
exitResult
The displacement history can be plotted as follows.
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