Simulating fracture of element
Posted: 07 Jul 2016, 22:06
Dear SeismoSoft team,
I perform static nonlinear analysis of a two-story steel special concentrically braced frame. I have made two models - first one with concentrated plasticity in a plastic hinge in the middle of the brace, in the second one I use the SeismoStruct v.7.0.6 infrmFB element and a Minegotto-Pinto steel material model for modelling bracing elements. To provoke buckling, an initial camber is applied in the middle of the brace.
After performing the analysis with monotonically increasing lateral displacements I got the resultant capacity curves. Both curves matches quite well with one difference in the plastic range - there is no falling branch in the curve for the model with distributed plasticity, that indicates loss of structural strength and stiffness rather it shows overstrength with increasing displacement of the control node.
I explain this effect with the fact that by modelling concentrated plasticity in a plastic hinge when reaching the accepted fracture criteria of the element, the strength of the element drops to zero but the analysis goes on with stress redistribution. That is not the case when using distributed plasticity.
Could you give me some advice about simulating fracture of element with loss of strength, which doesn't cause the analysis to stop but leading to stress redistribution and drop of stiffness and strength of the structure in the case of distributed plasticity?
Best regards,
Raycheva
I perform static nonlinear analysis of a two-story steel special concentrically braced frame. I have made two models - first one with concentrated plasticity in a plastic hinge in the middle of the brace, in the second one I use the SeismoStruct v.7.0.6 infrmFB element and a Minegotto-Pinto steel material model for modelling bracing elements. To provoke buckling, an initial camber is applied in the middle of the brace.
After performing the analysis with monotonically increasing lateral displacements I got the resultant capacity curves. Both curves matches quite well with one difference in the plastic range - there is no falling branch in the curve for the model with distributed plasticity, that indicates loss of structural strength and stiffness rather it shows overstrength with increasing displacement of the control node.
I explain this effect with the fact that by modelling concentrated plasticity in a plastic hinge when reaching the accepted fracture criteria of the element, the strength of the element drops to zero but the analysis goes on with stress redistribution. That is not the case when using distributed plasticity.
Could you give me some advice about simulating fracture of element with loss of strength, which doesn't cause the analysis to stop but leading to stress redistribution and drop of stiffness and strength of the structure in the case of distributed plasticity?
Best regards,
Raycheva