4. B modeling#
4.1. Characteristics of modeling#
In modeling B, the same calculation is made as in modeling A, but by decomposing it into a first part where the fluid potential associated with the modes of structure of the reservoir is explicitly obtained.
4.2. Tested sizes and results#
The added mass of the first mode is calculated by projecting the fluid displacement potential onto itself. The result is compared with that given by the operator CALC_MATR_AJOU.
Identification |
Reference Type |
Reference Value |
Tolerance |
Mass added from the first mode on itself |
“AUTRE_ASTER” |
96633 kg |
0.1% |
The pressure and speed potentials are then deduced by a factor \(\omega\) or \({\omega }^{2}\), \(\omega\) being the frequency of the mode in question.