3.2.6.2. DisplacementControl Commandο
This command is used to construct a DisplacementControl integrator object. In an analysis step with Displacement Control we seek to determine the time step that will result in a displacement increment for a particular degree-of-freedom at a node to be a prescribed value.
- integrator DisplacementControl $node $dof $incr <$numIter :math`\Delta U \text{min}` $:math:\Delta U \text{max}`>
Argument |
Type |
Description |
---|---|---|
$node |
integer |
node whose response controls solution |
$dof |
integer |
degree of freedom at the node; valid options: 1 through ndf at node. |
$incr |
float |
first displacement increment <math>Delta U_{text{dof}}</math> |
$numIter |
integer |
the number of iterations the user would like to occur in the solution algorithm. Optional; default = 1.0. |
$dUmin |
float |
the min step size the user will allow. optional; default \(\Delta U_{min} = \Delta U_0\) |
$dUmax |
float |
the max step size the user will allow. optional: default \(\Delta U_{max} = \Delta U_0\) |
\(f(x_n+\Delta x) = 0\)
integrator DisplacementControl 1 2 0.1; # displacement control algorithm seeking constant increment of 0.1 at node 1 at 2βnd dof.
3.2.6.2.1. Theoryο
If we write the governing finite element equation at :math:`t + Delta t` as:
where \(F(U_{t+\Delta t})\!\) are the internal forces which are a function of the displacements \(U_{t+\Delta t}\!\), \(F^{ext}\!\) is the set of reference loads and \(\lambda\!\) is the load multiplier. Linearizing the equation results in:
This equation represents n equations in \(n+1`\) unknowns, and so an additional equation is needed to solve the equation. For displacement control, we introduce a new constraint equation in which in each analysis step we set to ensure that the displacement increment for the degree-of-freedom <math>text{dof}</math> at the specified node is:
MORE TO COME:
In Displacement Control the \(\Delta_U\text{dof}\) set to \(t + \lambda_{t+1}\) where,
\(\Delta U_\text{dof}^{t+1} = \max \left ( \Delta U_{min}, \min \left ( \Delta U_\text{max}, \frac{\text{numIter}}{\text{lastNumIter}} \Delta U_\text{dof}^{t} \right ) \right )\)