Community Tip - Did you get an answer that solved your problem? Please mark it as an Accepted Solution so others with the same problem can find the answer easily. X
Hi ,
Version: Creo 2.0
perhaps this is a common problem in FEA models - I'm having trouble properly properly defining the rotational constraints in a model and I'm getting strange results because of it.
I would like to model a steel plate constrained with a pin joint on either side.
The plate should be loaded centrally with 5000N. (see pictures in Excel table).
What i expect to see is that the plate bends upwards in the middle and is free to rotate on either side until the plate comes into tension and holds the load.
The intention was to make a simple model to see if it behaves as intended and then i would use the same method on a more complicated assembly model.
I've ignored the stress levels at first and only looked at the displacements to see if the model is behaving as intended.
i've tried the following and none seem to give the right model behaviour:
The problem i see is that the pin/ball constraints seem to fix the edges and don't allow free rotation aroung the selected cylinderical surface as intended.
I thought the Cylindrical coord. system might work but it seems like i can allow any amount of rotational freedom and the resulting deflection just keeps on increasing with no end in sight.
would be great if someone had some more insights here - it doesn't seem to make sense.
Thanks,
Dermot
Solved! Go to Solution.
I went through your model and it looks like you're both constrain methods you previously tried did allow rotation (it's just a very small amount of rotation). I ran three different constraint methods: (1) pin constraint, (2) cylindrical coordinate system with theta free, and (3) a kinematic constraint with Rzz free. I also ran the methods (2) and (3) as a large displacement analysis (note that you can't run a LDA with a pin constraint and that I changed the load from a bearing load to a standard load as bearing loads aren't allowed for LDA); a screen show of displacement results for all 5 runs is shown below.
You'll notice that all methods have essentially identical results (the kinematic is a little smaller because the rigid link adds some stiffness to the model), and that the LDA models give above 10% higher displacements. Taking a closer look where the constraints were applied, we can clearly see that rotation is occurring (I zoomed into the top inside hole surface corner of the left lug). You can clearly see that node moves from it's original location for all methods except for the fixed.
To provide a little more clarification, I run method (2) and a fixed constraint with a moment measure on the constraint surface. For method (2), a moment of -3.157766e-08 Nmm was calculated, but for the fixed constraint a moment of -1.533312e+05 Nmm was calculated.
Now, at the end of the day, I think you and I are on the same page that the deformed shape doesn't "look right", as we'd expect to see larger rotations at the pin joint. I think part of the reason we're not seeing larger rotations is that the lugs effect the local bending stiffness of the plate, resulting in a change in the curvature of the bending.
Hi,
I haven't played with the pin / ball joints (I think they're new in Creo?) but I agree the results look weird.
Re the cylindrical csys, which I have used:
The most flexible and controllable approach is probably to create two points at each centre of rotation, one in the middle and one slightly offset. Link one to the surface with a Weighted Link, constrain the other in the DOFs you want (you can use the WCS for this; no need for a local csys unless the axis is at a strange angle), and connect the two points with an advanced spring, with sufficient stiffness not to influence your results unduly (but not too stiff otherwise the analysis may not converge). For your 5000 N, a linear stiffness of 1e7 would keep displacement to a quarter of a micron each, which you shouldn't notice.
Thanks for the input:
I've tried setting both R and Theta to 'free' - the error 'The model is insufficiently constrained for the analysis...' occurs.
We don't have an Advanced license so I can't use weighted links - I will try to constrain the model using points and springs to ground.
When I've tried out a few things I will know more.
I advise not using pin/ball constraints. I have documented them similar to what you are doing in your sheet and have noticed that their inclusion with any other type of link or constraint can and most likely will cause the memory requirements and solution time to increase dramatically. You will notice this during runtime in the .rpt file during the 'processing mulit-point constraints' step. I do not know why, and after getting comfortable with rigid and weighted links with springs and point constraints I feel they are, as Jonathan pointed out, less controllable and flexible anyway. We prefer to use weighted links or advanced rigid links along with springs to ground at points placed at the feature center. Then a point constraint applied allows rotational DOF. I also advise against the cylindrical csys approach as well due to the fact there are some circumstances were they are not supported for analyses.
Lastly when looking at your model it is rather thin and wide and if your displacements are large, it may quickly turn into a large deformation analysis which can have huge impacts on results.
Hope that helps and good luck,
- J -
Dermot,
If you want, you can post the model files and I can take a look at it. Looking over your Excel sheet, it's hard to see exactly how you set it up (as far as trying to find a mistake), but I do agree that it doesn't look like the contraint surfaces are rotation in Model 3.2 (even though Theta is set free). You could place a rotation measure there to see if it is really zero just to be on the safe side. Another option is to use rigid links to connect the inside surface to a datum point at the center, and then apply a constraint at said point with the correct rotational DOF released.
One more thing: it looks like you ran this as a linear analysis. Once the issues with the constraints are sorted out, you should run this as a large-displacement analysis.
Here's the model file - i tried to keep it as simple as possible.
Will try the suggestion with the rigid links to a central point in the rotational axis, the point then being constrained to allow rotation.
I went through your model and it looks like you're both constrain methods you previously tried did allow rotation (it's just a very small amount of rotation). I ran three different constraint methods: (1) pin constraint, (2) cylindrical coordinate system with theta free, and (3) a kinematic constraint with Rzz free. I also ran the methods (2) and (3) as a large displacement analysis (note that you can't run a LDA with a pin constraint and that I changed the load from a bearing load to a standard load as bearing loads aren't allowed for LDA); a screen show of displacement results for all 5 runs is shown below.
You'll notice that all methods have essentially identical results (the kinematic is a little smaller because the rigid link adds some stiffness to the model), and that the LDA models give above 10% higher displacements. Taking a closer look where the constraints were applied, we can clearly see that rotation is occurring (I zoomed into the top inside hole surface corner of the left lug). You can clearly see that node moves from it's original location for all methods except for the fixed.
To provide a little more clarification, I run method (2) and a fixed constraint with a moment measure on the constraint surface. For method (2), a moment of -3.157766e-08 Nmm was calculated, but for the fixed constraint a moment of -1.533312e+05 Nmm was calculated.
Now, at the end of the day, I think you and I are on the same page that the deformed shape doesn't "look right", as we'd expect to see larger rotations at the pin joint. I think part of the reason we're not seeing larger rotations is that the lugs effect the local bending stiffness of the plate, resulting in a change in the curvature of the bending.