Benchmark solution ===================== The analytical reference solution is determined by the theory of beams. We consider a freestanding embedded beam. The geometric characteristics are those defined in paragraph [:ref:`§2.1 <§2.1>`]. The prestressed cable applies a normal compression force :math:`(\mathrm{-}F;\mathrm{0 };0)` and a bending moment :math:`(\mathrm{0 };–\mathit{eF};0)` to the free end. The solution to this problem is as follows: **Stress tensor**: .. image:: images/Object_2.svg :width: 125 :height: 80 .. _RefImage_Object_2.svg: with .. image:: images/Object_3.svg :width: 125 :height: 80 .. _RefImage_Object_3.svg: **Travel:** .. image:: images/Object_4.svg :width: 125 :height: 80 .. _RefImage_Object_4.svg: with the **boundary conditions**: .. image:: images/Object_5.svg :width: 125 :height: 80 .. _RefImage_Object_5.svg: When the effects of Poisson are overlooked ( .. image:: images/Object_6.svg :width: 125 :height: 80 .. _RefImage_Object_6.svg: ), the travel solution is simplified as follows: .. image:: images/Object_7.svg :width: 125 :height: 80 .. _RefImage_Object_7.svg: The numerical reference values are calculated using the analytical expressions above, using for :math:`F` the overall equilibrium value of the normal force in the cable: .. image:: images/Object_8.svg :width: 125 :height: 80 .. _RefImage_Object_8.svg: