4. B modeling#
4.1. Characteristics of modeling#
Same as modeling A. Only the law of behavior changes: here the law is VISC_TAHERI.
4.2. Tested sizes and results#
Behavior VISC_TAHERI (with a time discretization 10 times finer than LEMAITRE)
Variables |
Moment (s) |
Reference |
Tolerance |
\({\varepsilon }_{{\nu }_{\mathrm{xx}}}\) |
30 |
1.762 10—4 |
|
\({\varepsilon }_{{\nu }_{\mathrm{xy}}}\) |
30 |
1.816 10—4 |
|
\({\varepsilon }_{{\nu }_{\mathrm{xx}}}\) |
3630 |
1.9030 10—3 |
|
\({\varepsilon }_{{\nu }_{\mathrm{xy}}}\) |
3630 |
2.0789 10—3 |
|
\({\varepsilon }_{{\nu }_{\mathrm{xx}}}\) |
3660 |
1.9130 10—3 |
|
\({\varepsilon }_{{\nu }_{\mathrm{xy}}}\) |
3660 |
2.1906 10—3 |
|
\({\varepsilon }_{{\nu }_{\mathrm{xx}}}\) |
3720 |
1.8740 10—3 |
|
\({\varepsilon }_{{\nu }_{\mathrm{xy}}}\) |
3720 |
3.1813 10—3 |
|
Note: the Brent method is used to solve the law of behavior.