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Nonlinear Elasto-Plastic Material Properties

Nonlinear material properties in LUSAS Modeller can be assembled by an appropriate combination of the elastic, plastic, creep, damage, etc. datasets. Details of the elasto-plastic material models available in LUSAS are presented in the following table.

Material Type

Model Name

Stress Potential Type

Yield Criteria

Model Number

Hardening Type

Stress Return Method

Different Tensile & Compressive Yield Stress?

Flow Rule

Isotropic Stress Resultant

-

von Mises (plastic moment)

29

Isotropic N/A

8

Associated
  Tresca

-

Tresca

61

Isotropic Explicit forward Euler

8

Associated
  Stress Potential

von Mises

von Mises

72

Isotropic Implicit backward Euler

8

Associated
   

Modified von Mises

von Mises

77

Nonlinear isotropic Implicit backward Euler

4

Associated
  Optimised Implicit von Mises

-

von Mises

75

Isotropic/

Kinematic

Steepest Descent (radial return)

8

Associated
  Mohr-Coulomb

-

Mohr-Coulomb

65

Isotropic Implicit backward Euler

8

Non-associated
  Drucker-Prager

-

Drucker-Prager

64

Isotropic Explicit forward Euler

8

Associated
  Cracking Concrete

-

Cracking Concrete

82

Isotropic Implicit backward Euler

8

Associated
Orthotropic Stress Potential

Hill

Hill

76

Nonlinear isotropic Implicit backward Euler

8

Associated
   

Hoffman

Hoffman

78

Nonlinear isotropic Implicit backward Euler

4

Associated
Specialised Interface

-

von Mises (normal)

Mohr Coulomb (shear

26, 27

Isotropic Steepest Descent

(sub-incrementation)

8

Associated

Notes:

  • See the LUSAS Theory Manual I ("Chapter 4.0: Constitutive Models" section) for more information on the terms used in the table
  • The stress return methods used for each material model cannot be manipulated. They are embedded in the material model
  • The column title "Different Yield Stress in Tension and Compression" means that not only is the specified yield stress assumed the same, but also any hardening characteristics
  • The kinematic input units are the same as those for the isotropic hardening (Force/Length2). Kinematic hardening not a parameter defined between 0 and 1, it is a kinematic hardening tangent and is available from experimental testing
  • Search for "Isotropic/Orthotropic Material Definition" in the online help for more general information on these material models
  • It is not possible to input a mathematical curve tp specify a nonlinear hardening response. Most of the models do, however, accept a piecewise-linear input
  • Note that, when the hardening behaviour is specified as a gradient, both the isotropic and kinematic hardening parameter need to be converted from the elasto-plastic modulus, Ep, to the slope of the uniaxial yield stress against equivalent plastic strain curve. Search for "Nonlinear Material Hardening Convention" in the online help for more information

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