Plane stress concept with a fixed end

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SUMMARY

The discussion centers on the applicability of plane stress theory in scenarios where one end of a 2D model is fixed. It is established that under fixed boundary conditions, the z-direction stress component cannot be zero, which contradicts the requirements of plane stress. The participants conclude that for plane stress to be valid when one end is fixed, shear must be applied at that boundary. They also provide numerical examples comparing stress results from 3D, 2D plane stress, and analytical models, demonstrating minimal differences in stress values.

PREREQUISITES
  • Understanding of plane stress and plane strain concepts
  • Familiarity with finite element analysis (FEA) techniques
  • Knowledge of stress and strain relationships in materials
  • Basic principles of elasticity and boundary conditions in structural analysis
NEXT STEPS
  • Study the principles of shear stress and its effects on boundary conditions
  • Learn about finite element modeling in software like ANSYS or Abaqus
  • Explore the differences between 2D and 3D stress analysis in structural engineering
  • Investigate the derivation and application of principal stress equations in elasticity
USEFUL FOR

Structural engineers, finite element analysts, and students studying mechanics of materials will benefit from this discussion, particularly those interested in the implications of boundary conditions on stress analysis.

feynman1
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Under plane stress (z direction perpendicular to the plane), there shouldn’t be any z stress component. Then if one end of the 2D model is fixed, does that mean the displacement on that fixed boundary is completely zero (u=v=w=0), but that will generally violate the stress component along z being 0.
 
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Sure.
 
Chestermiller said:
Sure.
is plane stress never applicable here under this BC?
 
feynman1 said:
is plane stress never applicable here under this BC?
How can it be? It requires the z principal stress and one other principal stress to be equal.
 
Chestermiller said:
How can it be? It requires the z principal stress and one other principal stress to be equal.
i don't get you by 'equal'
 
feynman1 said:
i don't get you by 'equal'
If the stretching were in the x-direction (i.e., BC applied at x = 0), the strains in the y- and z-directions would be zero. That would mean that the stresses in the y and z directions would have to be equal.
 
Chestermiller said:
If the stretching were in the x-direction (i.e., BC applied at x = 0), the strains in the y- and z-directions would be zero. That would mean that the stresses in the y and z directions would have to be equal.
'the strains in the y- and z-directions would be zero' for x=0 or for all x?
 
feynman1 said:
'the strains in the y- and z-directions would be zero' for x=0 or for all x?
At x = 0.
 
Chestermiller said:
At x = 0.
at x=0, stress y=stress z not equal to 0, because strain x isn't 0. but plane stress requires stress z to be 0.
 
  • #10
feynman1 said:
at x=0, stress y=stress z not equal to 0, because strain x isn't 0. but plane stress requires stress z to be 0.
Right
 
  • #11
Chestermiller said:
Right
but you seemed to disagree with plane stress being not applicable here.
 
  • #12
feynman1 said:
but you seemed to disagree with plane stress being not applicable here.
Sure. So...?
 
  • #13
Well, on 2nd thought, you can have a shear at the boundary like ##\partial v/\partial x## which would satisfy the requirement of plane strain.
 
  • #14
I don’t really understand this discussion. You can apply fixed constraint (all available DOFs* = 0) in plane stress finite element analysis. For example take a rectangular cantilever beam. Fix it at one end and apply load. Your software will give you correct stresses.

* all available DOFs - translations in X and Y direction (for some elememts also rotation about the Z axis), Z translation is simply not considered in 2D analysis
 
  • #15
In close proximity to the cantilever (say within a beam thickness), you don’t have plane strain. The beam equations are only an approximation to the full theory of elasticity equations.
 
  • #16
Let's consider an example - cantilever beam 1.5 m long, rectangular section 0.1x0.2 m. Loaded with 16000 N at the free end. Here are the results (maximum stress):
- 3D model: 36,98 MPa
- 2D plane stress model: 36,88 MPa
- beam model: 36,1 MPa
- analytical: 36 MPa
The only problem is with stress singularity caused by the unrealistic assumption of fixed constraint itself (both in case of 3D and 2D model) but it can be ignored and the results read slightly away from the very end of the beam.
 
  • #17
FEAnalyst said:
Let's consider an example - cantilever beam 1.5 m long, rectangular section 0.1x0.2 m. Loaded with 16000 N at the free end. Here are the results (maximum stress):
- 3D model: 36,98 MPa
- 2D plane stress model: 36,88 MPa
- beam model: 36,1 MPa
- analytical: 36 MPa
The only problem is with stress singularity caused by the unrealistic assumption of fixed constraint itself (both in case of 3D and 2D model) but it can be ignored and the results read slightly away from the very end of the beam.
we have been discussing the plane stress theory. of course these results differ little as you go away from the fixed end.
 
  • #18
Chestermiller said:
Sure. So...?
plane stress says stress z=0.
so is plane stress applicable here?
 
  • #19
feynman1 said:
plane stress says stress z=0.
so is plane stress applicable here?
As I said, it certainly applies to shear at the boundary you described.
 
  • #20
Chestermiller said:
As I said, it certainly applies to shear at the boundary you described.
but principal stress z is already not 0, violating plane stress requirements, why do we mention shear anyway?
 
  • #21
feynman1 said:
but principal stress z is already not 0, violating plane stress requirements, why do we mention shear anyway?
It is zero if we apply shear at your boundary.
 
  • #22
If the boundary is at x = 0, and u = w = 0, and ##v=\gamma x##, then, at the boundary, u = v = w = 0 and $$\sigma_{xx}=\sigma_{yy}=\sigma_{zz}=0$$ and $$\sigma_{xy}=G\gamma$$where G is the shear modulus. So we have plane strain throughout for this homogeneous deformation even though the principal in-plane stresses are not zero, even at the boundary.
 
  • #23
Chestermiller said:
If the boundary is at x = 0, and u = w = 0, and ##v=\gamma x##, then, at the boundary, u = v = w = 0 and $$\sigma_{xx}=\sigma_{yy}=\sigma_{zz}=0$$ and $$\sigma_{xy}=G\gamma$$where G is the shear modulus. So we have plane strain throughout for this homogeneous deformation even though the principal in-plane stresses are not zero, even at the boundary.
to fix the end with shear is really a brilliant idea of rendering the shaky plane stress applicable. but on 'the principal in-plane stresses are not zero, even at the boundary.', aren't the principal in-plane stresses 0 as you wrote in your equation?
 
  • #24
feynman1 said:
to fix the end with shear is really a brilliant idea of rendering the shaky plane stress applicable. but on 'the principal in-plane stresses are not zero, even at the boundary.', aren't the principal in-plane stresses 0 as you wrote in your equation?
Do you know how to determine the principal stresses for this specific state of stress? They are not zero. They are at two different angles to the boundary, offset from one another by 90 degrees.
 
  • #25
Chestermiller said:
Do you know how to determine the principal stresses for this specific state of stress? They are not zero. They are at two different angles to the boundary, offset from one another by 90 degrees.
sorry i got it wrong and the principal stresses aren't 0. then we can come to the conclusion that for plane stress to be applicable when 1 end is fixed, that fixed end has to be sheared.
 
  • #26
feynman1 said:
sorry i got it wrong and the principal stresses aren't 0. then we can come to the conclusion that for plane stress to be applicable when 1 end is fixed, that fixed end has to be sheared.
In-plane shear parallel to the boundary was the only way I was able to think of.
 

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