The stiffness of an FEA model depends on the mesh resolution?

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Discussion Overview

The discussion revolves around the relationship between mesh resolution and the stiffness of Finite Element Analysis (FEA) models. Participants explore theoretical aspects, mathematical derivations, and conceptual implications of mesh refinement on stiffness, including potential misunderstandings and historical perspectives.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that the stiffness of an FEA model decreases with a refined mesh, questioning the rigorous derivation of this claim.
  • One participant suggests constructing the stiffness matrix for a specific differential equation to observe changes as mesh size decreases.
  • Another participant expresses confusion about the relationship between mesh refinement and stiffness, asking for clarification on what exactly is decreasing.
  • Historical references to Galileo's work on scale invariance and material strength are introduced, though their relevance to the OP's question is debated.
  • Some participants mention shear locking as a related issue, but clarify that it is not the primary concern of the OP.
  • References to authoritative texts on FEA, such as works by Bathe and Hughes, are provided, indicating that mathematical proofs exist regarding the convergence behavior of FEA models.
  • One participant describes the concept of convergence from below, stating that displacements and stresses increase with mesh refinement, based on strain energy considerations.
  • Graphical representations of convergence and discretization are discussed, with participants sharing examples to illustrate their points.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the implications of mesh refinement on stiffness. Multiple competing views and interpretations of the relationship remain, with some participants seeking clarification and others providing differing perspectives.

Contextual Notes

There are unresolved questions regarding the definitions of stiffness in the context of FEA and the specific conditions under which mesh refinement affects stiffness. The discussion also touches on the potential for misunderstanding the implications of convergence in numerical methods.

Who May Find This Useful

This discussion may be of interest to those studying or working with finite element methods, particularly in the fields of engineering and applied mathematics, as well as individuals exploring the theoretical foundations of numerical analysis.

feynman1
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As is well known, the stiffness of an FEA model decreases with a refined mesh. What's the rigorous derivation of this?
 
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Why not construct the stiffness matrix for <br /> \frac{d^2u}{dx^2} = -f(x) for x \in (0,1) using elements [nh, h(n+1)] with basis functions <br /> \begin{split}<br /> f_0 : [0,h] \to \mathbb{R} : x &amp;\mapsto 1 - \frac{x}{h} \\<br /> f_1 : [0,h] \to \mathbb{R} : x &amp;\mapsto \frac{x}{h}<br /> \end{split} and see what happens as you reduce h?
 
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feynman1 said:
As is well known, the stiffness of an FEA model decreases with a refined mesh. What's the rigorous derivation of this?
Euhrm... sources?

Considering that the stiffness of the construction decreasing with mesh refinement would be really silly, do you mean the stiffness of the differential equation? But even in this case I'm not sure about this, why would this be true in general? So again: sources?
 
Instead of an admonishment I will provide a tangential and perhaps incorrect annswer.
I recommend Galileo Galilei "Two New Sciences" where one of which is scale invariance and the strength of materials . To my mind these arguments point directly quantum mechanics which set the scale by which big and small are tto be measured
I believe the examination of FEA issues withion scale of the simulation are really a recapitulation of Galileo's arguments about his brave new world. Read the original!

.
 
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hutchphd said:
Instead of an admonishment I will provide a tangential and perhaps incorrect annswer.
I recommend Galileo Galilei "Two New Sciences" where one of which is scale invariance and the strength of materials . To my mind these arguments point directly quantum mechanics which set the scale by which big and small are tto be measured
I believe the examination of FMEA issues withion scale of the simulation are really a recapitulation of Galileo's arguments about his brave new world. Read the original!

.

This answer and the relation to the OP's question is completely lost to me...
 
Arjan82 said:
This answer and the relation to the OP's question is completely lost to me...

My apologies. I was trying to be not very complete on purpose. I do not know the exact issues with FEA to which the OP alludes but my instinct is that they are related to issues of scale invariance vis. Galileo's discussion of scaling the size of animals and how the bones must modify shape). If one is not very careful issues of absolute scale can be changed with mesh size and subtle errors result. That Calileo fellow was pretty astute.
 
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Check the "Finite Element Procedures" by Bathe and "The Finite Element Method" by Hughes. There are mathematical proofs of that in these books.
 
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Arjan82 said:
Or does the OP mean shear locking?
no not shear locking in particular, though shear locking is due to stiffness being too high
 
  • #10
FEAnalyst said:
Check the "Finite Element Procedures" by Bathe and "The Finite Element Method" by Hughes. There are mathematical proofs of that in these books.
many thanks, could you tell which chapter in Bathe's book?
 
  • #11
feynman1 said:
many thanks, could you tell which chapter in Bathe's book?
It’s in the chapter 4.3. Convergence of analysis results. Especially paragraph 4.3.4. Properties of the Finite Element Solution.
 
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  • #12
feynman1 said:
As is well known, the stiffness of an FEA model decreases with a refined mesh. What's the rigorous derivation of this?
I recently worked through the derivation of the FEA model (with the help of @pasmith , thanks) and I know the term stiffness matrix goes back to mechanical engineering application dealing with the literal stiffness of materials but what do you mean when you say stiffness of an FEA model decreases. What is decreasing?

For example I derived the node equations for the differential equation

$$ \frac{d^2u(x)}{dx^2} = -f(x)$$

I got for linear test functions ##N_1(x) = \frac{x_2 - x}{\Delta{x}}## and ##N_2(x) = \frac{x - x_1}{\Delta{x}}##

$$\frac{1}{\Delta{x}}\begin{pmatrix}
1 & -1 \\
-1 & 1
\end{pmatrix}
\begin{pmatrix} u_1 \\ u_2 \end{pmatrix} \\
=
\begin{pmatrix}
- u_1' \\
u_2' \end{pmatrix} +
\begin{pmatrix}
\int_{x_1}^{x_2} N_1(x)f(x)\,dx \\
\int_{x_1}^{x_2} N_2(x)f(x)\,dx
\end{pmatrix}$$

So, as ##\Delta{x}## gets smaller, in what sense is the stiffness being reduced?
 
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  • #13
bob012345 said:
I recently worked through the derivation of the FEA model (with the help of @pasmith , thanks)
Is there a thread?
 
  • #14
  • #15
It sounds like it could be an interesting thread... :smile:
 
  • #16
bob012345 said:
what do you mean when you say stiffness of an FEA model decreases. What is decreasing?
What the OP meant is that FEM always converges from below (displacements and stresses increase with mesh refinement). This is proven in the aforementioned books, based on strain energy which is always underestimated in FEM.
 
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  • #17
FEAnalyst said:
What the OP meant is that FEM always converges from below (displacements and stresses increase with mesh refinement). This is proven in the aforementioned books, based on strain energy which is always underestimated in FEM.
Like this simple example of a 1D temperature profile of a rod of length 10 units where the red is the analytic solution, the points are the FEM numerical solution and the lines are the linear interpolations between the node values?

image.png
 
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  • #18
bob012345 said:
Like this simple example of a 1D temperature profile of a rod of length 10 units where the red is the analytic solution, the points are the FEM numerical solution and the lines are the linear interpolations between the node values?
Not really, such graphs are in fact commonly used to illustrate the concept of discretization. The plot showing what we discuss here (convergence from below) may look like this (from "A First Course in the Finite Element Method" by Logan):

plot.JPG
 
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  • #19
FEAnalyst said:
Not really, such graphs are in fact commonly used to illustrate the concept of discretization. The plot showing what we discuss here (convergence from below) may look like this (from "A First Course in the Finite Element Method" by Logan):

View attachment 298814
If I pick one point on my curve and plot the extrapolated solution vs. the number of elements used I get this where the red line is the exact value and the points are the extrapolated values between the node points for different numbers of elements;

desmos-graph (18).png
 
  • #20
bob012345 said:
I recently worked through the derivation of the FEA model (with the help of @pasmith , thanks) and I know the term stiffness matrix goes back to mechanical engineering application dealing with the literal stiffness of materials but what do you mean when you say stiffness of an FEA model decreases. What is decreasing?

For example I derived the node equations for the differential equation

$$ \frac{d^2u(x)}{dx^2} = -f(x)$$

I got for linear test functions ##N_1(x) = \frac{x_2 - x}{\Delta{x}}## and ##N_2(x) = \frac{x - x_1}{\Delta{x}}##

$$\frac{1}{\Delta{x}}\begin{pmatrix}
1 & -1 \\
-1 & 1
\end{pmatrix}
\begin{pmatrix} u_1 \\ u_2 \end{pmatrix} \\
=
\begin{pmatrix}
- u_1' \\
u_2' \end{pmatrix} +
\begin{pmatrix}
\int_{x_1}^{x_2} N_1(x)f(x)\,dx \\
\int_{x_1}^{x_2} N_2(x)f(x)\,dx
\end{pmatrix}$$

So, as ##\Delta{x}## gets smaller, in what sense is the stiffness being reduced?
same question from me, how to see the stiffness being reduced?
 
  • #21
FEAnalyst said:
It’s in the chapter 4.3. Convergence of analysis results. Especially paragraph 4.3.4. Properties of the Finite Element Solution.
many thanks really helpful, though it's not explained 100%, for all it says is that the solution is underestimated without saying why.
 
  • #22
feynman1 said:
many thanks really helpful, though it's not explained 100%, for all it says is that the solution is underestimated without saying why.
I didn't have time to go through the whole section carefully but I think that the explanation lies in the equations presented there and the text that you are talking about is just a comment to these equations.
 
  • #23
FEAnalyst said:
I didn't have time to go through the whole section carefully but I think that the explanation lies in the equations presented there and the text that you are talking about is just a comment to these equations.
I'm now looking for a comprehensible 2D example of a heated plate that I can learn and teach someone using the FEM analysis. I've looked but everything is either too complex and theoretical or uses triangular elements rather than square element which I need for a simple example by hand. Any suggestions would be appreciated.
 
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  • #24
I suggest that as an example you choose a problem that can be solved analytically and compare it to various FEM approaches . Start in 1D ?. Do this several times.
 
  • #25
hutchphd said:
I suggest that as an example you choose a problem that can be solved analytically and compare it to various FEM approaches . Start in 1D ?. Do this several times.
Thanks. That's a good suggestion but we did a couple different 1D examples both analytically solvable and now the student wants to see a 2D version.
 
  • #26
So go to 2D? Rectangular should be easy. Maybe circular? Hexagonal? (I don't know how nasty this will get). Nonorthogonal axis can be tricky.
 
  • #27
hutchphd said:
So go to 2D? Rectangular should be easy. Maybe circular? Hexagonal? (I don't know how nasty this will get). Nonorthogonal axis can be tricky.
I know. I want to avoid anything like those boundary value problems in Grad school.
 
  • #28
Life is messy. Physics a little less so.
 
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  • #29
pasmith said:
Why not construct the stiffness matrix for <br /> \frac{d^2u}{dx^2} = -f(x) for x \in (0,1) using elements [nh, h(n+1)] with basis functions <br /> \begin{split}<br /> f_0 : [0,h] \to \mathbb{R} : x &amp;\mapsto 1 - \frac{x}{h} \\<br /> f_1 : [0,h] \to \mathbb{R} : x &amp;\mapsto \frac{x}{h}<br /> \end{split} and see what happens as you reduce h?
what can we imply from this derivation?
 
  • #30
bob012345 said:
I'm now looking for a comprehensible 2D example of a heated plate that I can learn and teach someone using the FEM analysis. I've looked but everything is either too complex and theoretical or uses triangular elements rather than square element which I need for a simple example by hand. Any suggestions would be appreciated.
Check "A First Course in Finite Elements" book by Fish. You will find such example there.
 
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