Lame parameter mu = shear modulus derivation (rogue factor of 2)

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SUMMARY

The shear modulus \( G \) is equal to the Lame parameter \( \mu \) multiplied by 2, as derived from the isotropic stress-strain relationship: \( \sigma = \lambda \mathrm{tr}(\epsilon) \mathrm{I} + 2\mu \epsilon \). The confusion arises from the definition of shear strain, where the true shear strain is half of the engineering shear strain. This distinction is crucial for accurate tensor representation in material mechanics. The correct relationship is \( G = \frac{2\mu}{1} \), emphasizing the factor of 2 in the derivation.

PREREQUISITES
  • Understanding of linear, symmetric, isotropic stress-strain relationships
  • Familiarity with the concepts of shear modulus and Lame parameters
  • Knowledge of tensor notation and engineering shear strain
  • Basic principles of Hooke's law for isotropic materials
NEXT STEPS
  • Study the derivation of shear modulus from Lame's parameters in detail
  • Learn about the differences between true shear strain and engineering shear strain
  • Explore the implications of infinitesimal strain theory in material mechanics
  • Review Hooke's law applications in isotropic materials for practical examples
USEFUL FOR

Mechanical engineers, materials scientists, and students studying continuum mechanics will benefit from this discussion, particularly those focused on the relationships between stress, strain, and material properties.

Twigg
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Hello,

I am trying and failing to derive that the shear modulus ##G## is equal to the Lame parameter ##\mu##. I start with the linear, symmetric, isotropic stress-strain formula: $$\sigma = \lambda \mathrm{tr}(\epsilon) \mathrm{I} + 2\mu \epsilon$$ I then substitute a simple (symmetric) shear strain: $$\epsilon = \epsilon_{xy} (\hat{x} \otimes \hat{y} + \hat{y} \otimes \hat{x} )$$ But then I end up with $$\sigma_{xy} = 2\mu \epsilon_{xy}$$ or equivalently $$G = 2\mu$$ What did I goof up?

Thanks!
 
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