Benchmark solution ===================== Calculation method used for the reference solution -------------------------------------------------------- The critical pressure is given in [:ref:`bib1 `] or [:ref:`bib2 `] by the following expression: :math:`{P}_{\mathit{cr}}\mathrm{=}\frac{\mathit{Eh}}{R}\frac{1}{({n}^{2}+\frac{{b}^{2}}{2})}\left[\frac{1}{{(\frac{{n}^{2}}{{b}^{2}}+1)}^{2}}+\frac{{h}^{2}}{12{R}^{2}(1\mathrm{-}{\nu }^{2})}{({n}^{2}+{b}^{2})}^{2}\right]` .. csv-table:: "with", ":math:`b\mathrm{=}\frac{\pi R}{L}`" "", ":math:`n` represents the number of circumferential modes" This formula is valid in the case where :math:`N\mathrm{=}0.5R{p}_{\mathit{cr}}`. Benchmark results ---------------------- .. image:: images/Object_6.svg :width: 445 :height: 230 .. _RefImage_Object_6.svg: Uncertainties about the solution ---------------------------- Analytical solution Bibliographical references --------------------------- 1. S.P. TIMOSHENKO, J.M. GERE: Elastic Stability Theory, page 500, second edition, DUNOD 1966. 2. BO O. ALMROTH, D.O. BRUSH: Buckling of bars, plates and shells, page 173, Mc Graw-Hill, New York, 1975.