Using 2nd-Piola-Kirchoff stress rather than Cauchy

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SUMMARY

The discussion centers on the necessity of using the 2nd Piola-Kirchhoff stress tensor (S) instead of the Cauchy stress tensor (σ) in a general transport equation for materials. It is established that S and the Lagrangian strain tensor (E) form a work-conjugate pair, both being invariant to rigid body rotation, which is crucial for accurate constitutive relationships. The use of S is recommended for small strains, while σ, defined in a spatial reference frame, should not be used with E in constitutive equations. The conversation emphasizes the importance of selecting the appropriate stress tensor based on the context of the analysis.

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  • Understanding of 2nd Piola-Kirchhoff stress tensor (S)
  • Familiarity with Cauchy stress tensor (σ)
  • Knowledge of Lagrangian strain tensor (E)
  • Basic principles of Finite Element Analysis (FEA)
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  • Study the relationship between 2nd Piola-Kirchhoff stress and Cauchy stress
  • Explore the implications of using Lagrangian strain in constitutive relationships
  • Learn about the invariance of stress and strain tensors under rigid body rotation
  • Investigate rate-form constitutive relationships in material mechanics
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Engineers, researchers, and students involved in material mechanics, particularly those working with Finite Element Analysis (FEA) and stress-strain relationships in continuum mechanics.

hoomanya
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Hi,
I need to use the 2nd Piola Kirchoff Stress (S) rather than the usual Cauchy stress i(sigma) in a general transport equation of a material. I was wondering if I need to replace the stress tensor (usually denoted by sigma) with S, or do I just write sigma in terms of S using the relationship that exists between S and sigma.
Thanks!
 
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I see you have no responses, so I'll give you something to think about -- though, I speak from an FEA standpoint:

Why do you NEED to use the PKII stress, S?
Is it because you are using the Lagrangian Strain tensor, E?

Your stress and strain pair (constitutive relationship - e.x. Hooke's Law) must be work- conjugate, meaning that they must behave the same under rigid body rotation. The PKII stress tensor, S, and the Lagrangian strain tensor, E, are indeed both invariant to rigid body rotation, so they are a work-conjugate pair.

S is only meaningful for small (infinitesimal) strains. You could potentially acquire the Cauchy stress, \sigma, from S, as you describe -- but you wouldn't want to use \sigma with E in your constitutive relationship. Keep in mind that \sigma is defined in in a spatial reference frame (it is defined in your original coordinate system, regardless of whether there is rigid body rotation).

If your constitutive relationship is in rate-form, then that's a whole 'nother story.

Also, I remind you that I am an FEA guy, so if nothing I said applies to you, I apologize.
 
Thanks. What you said made sense. I also had a read of the wiki page on stress and am a lot more clear now.
 

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