dozer
Structural
- Apr 9, 2001
- 506
I've been playing with COSMOS/M using it to analyze a simple truss with a uniform gravity load on the bottom chord. Simple hand calcs indicate that the center of the top chord will be the critical element and it will buckle in the inelastic range. I ran a linear buckling analysis and got an eigenvalue that agreed very close with what I would have got if I checked the chord as though it were in the elastic range.
I want to understand what "really" happens but not being very familiar with nonlinear buckling analysis, I farmed it out. This analysis (using ABAQUS, spelled?)indicated a load factor at failure (ie; muliplier on load that caused buckling) slight higher than the eigen solution. What puzzles me is I would have expected a slightly lower value because I thought it was going to be in the inelastic range and the chord failed at its yield strength which suggest to me it didn't fail by buckling at all. (Yes, material nonlinearity was included.)
Here's my question, can a nonlinear analysis accurately predict inelastic buckling? If so, what is the secret to getting it to do so?
At the risk of boring you let me add to my description. One of the things I'm really trying to get my brain around is reasonable k-values for truss members. Text I've read recommend a value of one for chords, the theory being that if a member adjacent to another member wants to buckle at the same time it will offer no rotational stiffness at the joint. When I ran the linear buckling this is exactly what the deflected shape indicated. The top chord to the left of center buckled one way, the adjacent chord to the right of the joint buckled the other. Thus the joint that was common to both of these members rotated. This makes perfect sense to me but the nonlinear analysis I had run is not showing this. My fear is my managers will look at this nonlinear analysis and say "See, you can use a k much lower than one." But physically I just don't believe it. My suspicion is one or both of the following:
1) The program is not doing inelastic buckling correctly. (Hence my original question.)
2) The program is not accounting for the loss of stiffness when two adjacent members are loaded at the same level.
Thanks in advance,
Randy
I want to understand what "really" happens but not being very familiar with nonlinear buckling analysis, I farmed it out. This analysis (using ABAQUS, spelled?)indicated a load factor at failure (ie; muliplier on load that caused buckling) slight higher than the eigen solution. What puzzles me is I would have expected a slightly lower value because I thought it was going to be in the inelastic range and the chord failed at its yield strength which suggest to me it didn't fail by buckling at all. (Yes, material nonlinearity was included.)
Here's my question, can a nonlinear analysis accurately predict inelastic buckling? If so, what is the secret to getting it to do so?
At the risk of boring you let me add to my description. One of the things I'm really trying to get my brain around is reasonable k-values for truss members. Text I've read recommend a value of one for chords, the theory being that if a member adjacent to another member wants to buckle at the same time it will offer no rotational stiffness at the joint. When I ran the linear buckling this is exactly what the deflected shape indicated. The top chord to the left of center buckled one way, the adjacent chord to the right of the joint buckled the other. Thus the joint that was common to both of these members rotated. This makes perfect sense to me but the nonlinear analysis I had run is not showing this. My fear is my managers will look at this nonlinear analysis and say "See, you can use a k much lower than one." But physically I just don't believe it. My suspicion is one or both of the following:
1) The program is not doing inelastic buckling correctly. (Hence my original question.)
2) The program is not accounting for the loss of stiffness when two adjacent members are loaded at the same level.
Thanks in advance,
Randy