Understanding the strain energy function invariant term

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Discussion Overview

The discussion centers on understanding the strain energy function invariant terms, specifically focusing on the definitions and implications of the invariants I1 and I4 derived from Green's strain tensor in the context of large deformations. Participants explore the relationships between these invariants, the stretch ratios, and the role of unit vectors in the formulation.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions whether I4 can be concluded to consist of a unit vector multiplied by the principal stretch.
  • Another participant identifies λ1, λ2, and λ3 as "normal stretch" and suggests they are stretch coefficients aligned with the normal plane vector.
  • A participant seeks clarification on whether the components N1, N2, and N3 of the unit vector should always equal 1 or if they can vary under different conditions.
  • There is a discussion about the differentiation between left and right stretch tensors, with one participant expressing uncertainty in evaluating this distinction.
  • A later reply confirms that N_i is a unit vector, emphasizing that while its magnitude is always 1, its direction can vary based on the local context.

Areas of Agreement / Disagreement

Participants express varying interpretations of the definitions and roles of the invariants and unit vectors, indicating that multiple competing views remain without a clear consensus on certain aspects.

Contextual Notes

There are unresolved questions regarding the conditions under which the components of the unit vector may change and the differentiation between left and right stretch tensors, which could affect the understanding of the strain energy function.

fruitkiwi
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Hi, Dear all,

Facing problem to understand strain energy function invariant terms
A typical strain energy function consist of strain invariant can be defined as followed
W(I1,I4)=C0+C1(I1-3)(I4-1)+C2(I1-3)^2+C3(I1-4)^2+C4(I1-3)+C5(I4-1),
I1 and I4 are so called invariants of Green's strain tensor. (large deformation)
I1=trC=λ1^2+λ2^2+λ3^2
I4=N1*λ1^2*N1+N2*λ2^2*N2+N3*λ3^2*N3.

here is the complete link taken http://www.engin.umich.edu/class/bme456/ch6fitelasticmodelconstant/bme456fitmodel.htm

1. I read from article that N is a unit vector along the stretch direction, so can i conclude that
I4 consist of unit vector multiply with principal stretch?

2. the lamda in the formula is stretch ratio or principal stretch?
 
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After giving it a quick read,

2)\lambda_1 ,\lambda_2 ,\lambda_3 are the "normal stretch", where the link calls them that. but I think they are just the stretch coefficients for force in the same direction as the normal plane vector.

1) Yes, It seems so then, assuming you have "principle"\iff"normal"

That's my take on it.
 
jfy4 said:
After giving it a quick read,

2)\lambda_1 ,\lambda_2 ,\lambda_3 are the "normal stretch", where the link calls them that. but I think they are just the stretch coefficients for force in the same direction as the normal plane vector.

1) Yes, It seems so then, assuming you have "principle"\iff"normal"

That's my take on it.

Hi, jfy4,

I actually try to read more, but cannot find resources.
1. so all the N1, N2, N3,should always equal to 1? or under any condition they will change?
2. or can I call them as right stretch tensor?sorry, as i cannot differentiate left and right stretch tensor, so cannot evaluate more for you.
 
well, N_i is a unit vector, a vector whose magnitude is 1. That is N_i N_i=N_{1}^{2}+N_{2}^{2}+N_{3}^{2}=1. But, it is a vector, not a constant, so it's direction can vary. It says:
where N_i are the components of the unit vector aligned along the local muscle fiber direction.
 

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