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Solution Method
By using a first order finite difference approximation wit step size
6.57 get the form
 |
(168) |
and
 |
(169) |
where
is the stress at the precious time step. With
 |
(170) |
we have
 |
(171) |
where
with  |
(172) |
The upper bound
makes sure that yield condtion 6.63 holds. With this setting the eqaution 6.69 takes the form
 |
(173) |
After inserting 6.73 into 6.64 we get
 |
(174) |
Combining this with the incomressibilty condition 6.56 we need to solve a
Stokes problem as discussed in section 6.1.1 in each time step.
If we set
 |
(175) |
we need to solve the nonlinear problem
 |
(176) |
We use the Newton-Raphson Scheme to solve this problem
 |
(177) |
where
denotes the derivative of
with respect of
and
.
Looking at the evaluation of
in 6.75 it makes sense formulate
the iteration 6.77 using
.
In fact we have
with  |
(178) |
As
 |
(179) |
we have
with  |
(180) |
which leads to
 |
(181) |
Next: Functions
Up: Isotropic Kelvin Material
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