Algebraic Inversion of Stress-Strain Relations?

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Discussion Overview

The discussion revolves around the algebraic inversion of stress-strain relations, particularly focusing on deriving stress equations from strain equations and vice versa. The scope includes theoretical aspects of linear elasticity and viscoelasticity, as well as matrix representations of these relations.

Discussion Character

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

Main Points Raised

  • One participant inquires about the method for deriving stress equations from strain equations, seeking clarity on the inversion process.
  • Another participant provides specific stress-strain relations for linear elasticity, suggesting that inversion is discussed in a referenced text but expresses confusion about the details of the inversion process.
  • A different participant proposes a matrix approach to represent the stress-strain equations, indicating that inversion is straightforward for isotropic solids and outlines a method involving matrix manipulation.
  • Further, a participant raises concerns about incorporating additional terms into the matrix formulation, specifically questioning how to handle terms that involve stress itself in the matrix equation.

Areas of Agreement / Disagreement

Participants express varying levels of understanding regarding the inversion process, with some proposing methods while others remain uncertain about specific terms and their treatment in the matrix formulation. No consensus is reached on the best approach to handle the additional terms in the viscoelastic stress-strain relation.

Contextual Notes

Participants highlight potential complexities in the inversion process, particularly with terms that involve stress and time-dependent behavior, indicating that the treatment of these terms may require unique considerations or matrices.

Hypatio
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How is this accomplished? How can one derive equations for stress in terms of strain from equations of strain in terms of stress or vice versa?
 
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Which particular relations are you thinking of?
 
Studiot said:
Which particular relations are you thinking of?
I think that the stress-strain relations for linear elasticity are

\sigma_{ij}=\lambda \epsilon_{kk} +2\mu\epsilon_{ij}
and
\epsilon_{ij}=\frac{1+v}{E}\sigma_{ij}-\frac{v}{E}\sigma_{kk}

Inversion is briefly discussed in 'section' 3.2.8 here:

http://solidmechanics.org/text/Chapter3_2/Chapter3_2.htm

but I do not comprehend how exactly the inversion is performed

My actual goal is to invert the viscoelastic stress-strain relation here:

\dot{\sigma_{ij}}+\frac{\mu}{\eta}\sigma_{ij}=2\mu\dot{\epsilon_{ij}}+\delta_{ij}\left [ \lambda\dot{\epsilon_{kk}}-k\alpha_V \dot{T}+k\frac{\mu}{\eta}(\epsilon_{kk}-\alpha_V T) \right ]

which obviously has some additional terms. But I'm not sure how trivial this is.
 
Last edited:
The basic idea is to write the stress-strain equations as a 6x6 matrix equation

\varepsilon = D \sigma

and then invert the matrix. The matrix inversion is easy for an isotropic solid.

For the thermal example in your link, you then write the complete equation in matrix form

\varepsilon = D \sigma + A \Delta t

where A is a vector. Then

D^{-1} \varepsilon = \sigma + D^{-1} A \Delta t

which is usually written as

C \varepsilon = \sigma + C A \Delta t

so

\sigma = C \varepsilon - C A \Delta t

And you can multiply out CA to get the equations in your link.
 
Thanks, although I'm not sure how to treat some of the other terms which appear here:

\sigma_{ij}=2\mu\epsilon_{ij}+\epsilon\lambda+\delta_{ij}\left [\epsilonk\int_0^t\frac{\mu}{\eta}dt-k\alpha_V T-k\int_0^t\alpha_V\dot{T}\frac{\mu}{\eta}dt-\int_0^t\sigma_{ij}\frac{\mu}{\eta}dt \right ]

Can all of the terms be introduced into the same matrix C=D^{-1} as you have done with k\alpha_V T or do they have to be described with a unique matrix? I'm specifically unsure about how to deal with the last term in which \sigma_{ij} appears. How is this introduced into the matrix formula?

Thanks again.
 

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