Continuum Mechanics: Eij and eif given coordinates and displacements

Click For Summary
SUMMARY

The discussion focuses on the calculation of the Lagrangian strain tensor \(E_{ij}\) and the infinitesimal strain tensor \(\epsilon_{ij}\) in the context of continuum mechanics, specifically given coordinates and displacements. The correct formulas for these tensors are provided, emphasizing that they depend on the original coordinates \(X\) rather than the deformed coordinates \(x\). The user initially attempted to construct a displacement field but was advised to ensure that the displacement components \(u\) and \(v\) are functions of the original coordinates \(X_1\) and \(X_2\) in a 2D context.

PREREQUISITES
  • Understanding of continuum mechanics principles
  • Familiarity with strain tensor definitions and calculations
  • Knowledge of partial derivatives in multivariable calculus
  • Basic grasp of 2D coordinate systems in mechanics
NEXT STEPS
  • Study the derivation and application of Lagrangian strain tensors in continuum mechanics
  • Learn about the differences between Lagrangian and Eulerian strain measures
  • Explore the use of displacement fields in finite element analysis (FEA)
  • Investigate the implications of coordinate transformations on strain calculations
USEFUL FOR

Students and professionals in mechanical engineering, civil engineering, and applied physics, particularly those focusing on material deformation and structural analysis.

lanew
Messages
12
Reaction score
0

Homework Statement


http://imageshack.us/photo/my-images/513/selection027.png"
http://imageshack.us/photo/my-images/513/selection027.png

Homework Equations


[itex]E_{ij}=\frac{1}{2} \left( \frac{\partial{u_i}}{\partial{X_j}} \frac{\partial{u_j}}{\partial{X_i}} - \delta_{ij}\right)[/itex]
[itex]\epsilon_{ij}=\frac{1}{2}\left(\frac{\partial{u_i}}{\partial{X_j}}+\frac{\partial{u_j}}{\partial{X_i}}\right)[/itex]

The Attempt at a Solution


I'm not exactly sure where to begin. I understand how to find [itex]E_{ij}[/itex] and [itex]\epsilon_{ij}[/itex] given the displacement field, but I am not sure how to construct the field. So far, I came up with:

[itex]u=0.001x_1+0.003x_2+0.002x_3[/itex]
[itex]v=0.002x_2+0.001x_3-0.001x_4[/itex]

But I'm not sure that's right at all, or if I'm supposed to be looking at each individual point, e.g.:

[itex]u_1=0.001x_1[/itex]
[itex]v_1=0[/itex]

[itex]u_2=0.003x_2[/itex]
[itex]v_2=0.002y_2[/itex]

[itex]u_3=0.002x_3[/itex]
[itex]v_3=0.001y_3[/itex]

[itex]u_4=0[/itex]
[itex]v_4=-0.001y_4[/itex]

Am I even remotely close with either idea?

Thanks!
 
Last edited by a moderator:
Physics news on Phys.org
lanew said:
Am I even remotely close with either idea?

Thanks!

Not really, sorry..

Your problem appears to be 2D.
Furthermore, the two strain tensors that you want to find are Lagrangian and so, by definition, depend on capital [itex]X[/itex], rather than x...

Unless I misread the problem, you ought to take [itex]X_1=``x''[/itex] and [itex]X_2=``y''[/itex] (that's it.. because it's 2D).

[itex]u[/itex] and [itex]v[/itex] should depend on [itex]X_1[/itex] and [itex]X_2[/itex].

You have to figure out the relationship..

I'd also double check your formula:
Should read:
[itex]E_{ij}=\frac{1}{2}(\frac{\partial u_i}{\partial X_j}+\frac{\partial u_j}{\partial X_i}+\frac{\partial u_k }{\partial X_i}\frac{\partial u_k}{\partial X_j})[/itex]
Hope that helps..
 
Last edited:

Similar threads

  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 5 ·
Replies
5
Views
4K
  • · Replies 14 ·
Replies
14
Views
7K
  • · Replies 35 ·
2
Replies
35
Views
30K