User:JoKalliauer/gallery

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Sun May 12 21:08:16 CEST 2019

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Sun May 12 20:56:17 CEST 2019

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2017-11-04 22:05:00

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  • Boundary conditions of the quatermodel Boundary conditions of uniaxial stress
    Boundary conditions of the quatermodel
    Boundary conditions of uniaxial stress
  • preliminary analysis, modelling the material as linear elastic NLGEOM=NO Strech in loading direction: ϵ₁₁,nom=1
    preliminary analysis, modelling the material as linear elastic NLGEOM=NO
    Strech in loading direction: ϵ₁₁,nom=1
  • preliminary analysis, modelling the material as linear elastic NLGEOM=NO Strech orthongonal to the loading direction: ϵ₂₂,nom=-0.49
    preliminary analysis, modelling the material as linear elastic NLGEOM=NO
    Strech orthongonal to the loading direction: ϵ₂₂,nom=-0.49
  • preliminary analysis, modelling the material as linear elastic NLGEOM=NO Stresses in loading direction: σ₁₁=3MPa
    preliminary analysis, modelling the material as linear elastic NLGEOM=NO
    Stresses in loading direction: σ₁₁=3MPa
  • preliminary analysis, modelling the material as linear elastic NLGEOM=NO Displacement in loading direction: u₁
    preliminary analysis, modelling the material as linear elastic NLGEOM=NO
    Displacement in loading direction: u₁
  • preliminary analysis, modelling the material as linear elastic NLGEOM=NO Displacement orthonogal to the loading direction: u₂
    preliminary analysis, modelling the material as linear elastic NLGEOM=NO
    Displacement orthonogal to the loading direction: u₂
  • preliminary analysis, modelling the material as linear elastic NLGEOM=YES logaritmic strain in loading direction: ϵ₁₁,log=ln(2)~0.6931
    preliminary analysis, modelling the material as linear elastic NLGEOM=YES
    logaritmic strain in loading direction: ϵ₁₁,log=ln(2)~0.6931
  • preliminary analysis, modelling the material as linear elastic NLGEOM=YES logaritmic strain orthongolal to the loading direction: ϵ₂₂,log=-0.49*ln(2)~-0.3396
    preliminary analysis, modelling the material as linear elastic NLGEOM=YES
    logaritmic strain orthongolal to the loading direction: ϵ₂₂,log=-0.49*ln(2)~-0.3396
  • preliminary analysis, modelling the material as linear elastic NLGEOM=YES Stesses in loading direcition (using logaritmic strains): σ₁₁=3*ln(2)~2.070MPa
    preliminary analysis, modelling the material as linear elastic NLGEOM=YES
    Stesses in loading direcition (using logaritmic strains): σ₁₁=3*ln(2)~2.070MPa
  • preliminary analysis, modelling the material as linear elastic NLGEOM=YES Displacement in loading direction (using logaritmic strains): u₁
    preliminary analysis, modelling the material as linear elastic NLGEOM=YES
    Displacement in loading direction (using logaritmic strains): u₁
  • preliminary analysis, modelling the material as linear elastic NLGEOM=YES Displacement orthogonal to the loading direction (using logaritmic strains): u₂
    preliminary analysis, modelling the material as linear elastic NLGEOM=YES
    Displacement orthogonal to the loading direction (using logaritmic strains): u₂
  • Ogden hyperelastic material Logaritmic strain in loading direction: ϵ₁₁,log~0.6931
    Ogden hyperelastic material
    Logaritmic strain in loading direction: ϵ₁₁,log~0.6931
  • Ogden hyperelastic material Logaritmic strain orthogonal to the loading direction: ϵ₂₂,log~-0.2328
    Ogden hyperelastic material
    Logaritmic strain orthogonal to the loading direction: ϵ₂₂,log~-0.2328
  • Ogden hyperelastic material Logaritmic strain in loading direction: σ₁₁~1.534MPa
    Ogden hyperelastic material
    Logaritmic strain in loading direction: σ₁₁~1.534MPa
  • Ogden hyperelastic material Displacements in loading direction: u₁
    Ogden hyperelastic material
    Displacements in loading direction: u₁
  • Ogden hyperelastic material Displacements orthogonal to the loading direction: u₂
    Ogden hyperelastic material
    Displacements orthogonal to the loading direction: u₂
  • Represantiv volume Element under uniaxial stress.
    Represantiv volume Element under uniaxial stress.

2017-11-05 18:27:43

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