In this article I will put a compelling argument forward why glued meshes (with a gap) are a much better option that the more traditional stitched mesh approach for modelling thin plate structures with 2D shell elements.
The Compromise
FEA analysts still often represent thin solid parts using 2D (shell) elements with a thickness property as an economical alternative to modelling the thin parts using actual solid elements, as shown in Figure 1 below, despite a number of known disadvantages.
When modelling a structure like the typical example shown above [Figure 1], it is quite clear that using solid elements to represent the plates, with at least 2 elements through the thickness, is not a feasible option (unless you require the additional detail for a specific reason, or you have lots of storage space and time on your hands).
One of the known disadvantages of shell element models though, which many analysts have knowingly lived with in favour of the computational advantage these models have over solid element models, is the fact that mathematically there exist duplicate material at T-junctions where such elements meet. In a typical T-joint as shown below [Figure 2], the surfaces are extended until they intersect to ensure a connection that allows load transfer between the elements, but it does not take into account that in reality the connection is on the surfaces of those thick sections.
Visually, such a mesh looks like the image above on the left with a proper connection, while mathematically, it represents what is shown on the right, with an effective material overlap in the T-junction area.
The glue sceptics
The above compromise was for a very long time an acceptable one since FEA has always been understood to be an approximation method. Glue contact, when used with the half thickness gap present, is now an even better and more reliable alternative to use, but traditional analysts are still quite sceptical about the glue contact approach, so lets compare these two.
Glue contact explained
In the glue contact approach, surfaces are not extended to connect physically and therefore retains a gap in the model as shown below [Figure 3] which eliminates any duplicate material, but using an automated approach, those elements are however mathematically connected through what we term "glue contact".
Figure 3: Glued (un-stitched) meshes with thickness property (rendered in 3D on the right). In MSC Apex the glued elements are rendered as such (on the left) in the pre-processing phase.
It is important to note that the thickness property dictates whether or not the elements should be connected and secondly, it determines how many elements over the width of the connection should be connected (compare the deformed shape of the bottom plates in the results further down in this study).
The glue sceptics explained
The sceptics have a number of reasons why not to use glue contact and why to continue using stitched meshes, despite the known disadvantages:
Why consider glue contact?
While the arguments against glue contact is rapidly evaporating with recent advances in FE solver technology and user interface improvements, it should not be evaluated on these arguments alone. It should first be said that the traditional method of stitched meshing did not become the norm as opposed to the glue contact method, but in the absence of glue contact technology. Glue contact was only developed much later and until recently, was really difficult to get to work. You might even say that early attempts at introducing glue contact may have given it a bad reputation.
But the advantages that glue contact promised was incentive enough to justify its further development as shown in these pro-glue contact arguments:
Comparing the different methods
In this demonstration (see Figure 4 below), the stiffnesses of different parts using different element types and mesh densities, but representing the same structure, were compared. The parts in Figure 4 were setup as follows:
The only difference between the top row of parts (1 to 4) and their corresponding bottom row parts (5 to 8) are their respective mesh densities. Parts 1 to 4 have higher mesh densities than parts 5 to 8.
As a benchmark, the shell element parts were compared to the solid meshes (which are traditionally considered to be the most accurate).
The reason different mesh sizes and solid element types were introduced in the benchmark was to also show the relative sensitivity of the results to such differences when comparing the results from the different shell meshes to these solid parts.
Figure 4: Comparing eight different meshes representing the same T-section. Parts 1 to 4 has double the mesh density of Parts 5 to 8.
For the stiffness comparison, a normal modes analysis was used since $latex w_{n}=\sqrt{k/m} $ with $latex w_{n}$ measured in [rad/s] which means that the natural frequency of the parts is directly and only affected by the stiffness and mass of the structure. Although we know that parts 2 and 6 in Figure 4 are slightly heavier due to the small portions of duplicate mass, the other parts are identical in weight and therefore any difference in natural frequency is a direct measure of difference in stiffness.
To quantify the influence of the mass difference (3.76%) on the natural frequencies of parts 2 and 6 compared to those of the others, assuming equal stiffness, the natural frequencies of parts 2 and 6 should be 1.83% lower than the others due to the additional mass alone based on our simple equation for natural frequencies.
Therefore, any difference in natural frequency of more or less than 1.83% between parts 2 as well as 6 and the rest of the parts, can only be attributed to a difference in stiffness since the the same material was defined for all the parts.
To emphasize the effect of the connection stiffness, the parts were constrained as follows: The top and left most edges of the T-sections were constrained while leaving one edge free on each (see Figure 5). The first and second mode shape results shown in figures 6 and 7 show the effect of the chosen constraints.
Before we compare the stitched versus glue results, Figure 8 shows the advantage that shell meshes have above solid meshes when comparing solving times (especially for the small element meshes).
Figure 8 shows a recording of the solution times of the various parts, normalised to the quickest running part, part 7 (the stitched coarser shell element mesh).
From the above solution time results it can be seen that the finer Tet10 element mesh took the longest to solve (almost 4 times longer) due to its large number of nodes and there was indeed a premium paid for the solution time of the glued parts versus the stitched parts, although only in the region of 2.9% (when comparing the solving times of Part 1 to Part 2 and Part 5 to Part 6).
The most important comparison however is below in Table 1 when comparing the actual results (in Hertz) between the different parts. These results show that the stitched meshes are far less stiff than the other meshes.
To put the differences between these values in perspective, here are the results in graph form with frequency along the bottom axis:From the results shown in Table 1 the stitched meshes for both mesh densities under predict the natural frequencies by up to 20%, compared to the average solid mesh results, while the glued meshes predict the frequencies to within 0.7%. To put that in perspective, the impact of the glued meshes compared to the solid meshes, are less than the impact of the mesh densities between the same solid meshes alone!
Figure 9 shows the results of table 1 normalised to the average of the solid mesh results.
From the above stiffness impact results it can be seen that the stitched models consistently under predicts the stiffness compared to the other meshes.
But why is the glued method so much more accurate than the stitched method?
The answer to this question can be illustrated using Figure 10 below.
The reason why the stiffness of the glued meshes are on par with that of the solid meshes are because the thicknesses of the connecting plates are taken into account in the "footprint" of the glue contact. In Figure 10, the bottom plate bending pattern of both the glued and solid meshes clearly shows the effect of the vertical plate's thickness.
When comparing that to the stitched mesh plate bending, the bottom plate's bending is not affected by the vertical plate's thickness and therefore is much less stiff (up to 20% less stiff in this comparison).
In conclusion
It is true that the shown error above between stitched meshes and glued meshes becomes less severe with larger plate length to thickness ratios but there is yet one other aspect to take into account: Model preparation time.
When solving a model with solid elements are not an option, creating a stitched mid-surface mesh is far more time consuming than a glued mid-surface mesh.
The reasons to support my claim that glued meshes are far better to use than stitched meshes, are:
In short, the only disadvantage glued meshes have over stitched meshes, is history!