Benchmark solution ===================== Calculation method used for the reference solution -------------------------------------------------------- The aim of the reference solution is to analytically calculate the threshold value at which creep occurs. Some non-regression results on the movements at the last time step are added to verify the overall rigidity of the system. For the analytical calculation of the threshold we have: As long as the structure remains elastic and due to the boundary conditions, the stress tensor is written as: For the first time step between :math:`0` and :math:`106s` .. image:: images/Object_1.svg :width: 122 :height: 28 .. _RefImage_Object_1.svg: , and in second and .. image:: images/Object_2.svg :width: 122 :height: 28 .. _RefImage_Object_2.svg: in :math:`\mathrm{MPa}`. The other components of the tensor are zero. For the others no time, .. image:: images/Object_3.svg :width: 122 :height: 28 .. _RefImage_Object_3.svg: But we have: .. image:: images/Object_4.svg :width: 122 :height: 28 .. _RefImage_Object_4.svg: Let it be as in this case .. image:: images/Object_5.svg :width: 122 :height: 28 .. _RefImage_Object_5.svg: , we obtain immediately by solving :math:`D=1` the value of the time from which the creep occurs: :math:`{t}_{1}=4.08181818{10}^{6}s` Thus for a time equal to :math:`{t}_{1}`, the viscous deformations are zero and :math:`D` is equal to 1. Benchmark results ---------------------- Internal variable :math:`\mathrm{V1}` and :math:`\mathrm{V2}` at the point :math:`A`, :math:`B`, :math:`C` and :math:`E` as well as the movement from point :math:`B` to the last time step Bibliographical references --------------------------- 1. P. DE BONNIERES: Integrating viscoelastic relationships in STAT_NON_LINE [:ref:`R5.03.08 `] February 2001