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multiPlas - Dynardo GmbH

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3 THEORY OF THE MULTIPLAS MATERIAL MODELS IN ANSYS<br />

3.1 Basics of elasto-plasticity in <strong>multiPlas</strong><br />

The material models in <strong>multiPlas</strong> uses a rate-independent plasticity. The material models are characterized<br />

by the irreversible strain that occurs once yield criteria are violated. It is assumed that the total strain<br />

vector can be divided into a elastic and a plastic component.<br />

where:<br />

{ } { } { } pl<br />

el<br />

tot<br />

ε ε + ε<br />

= (3-1)<br />

{ε} el – elastic strain vector (EPEL)<br />

{ε} pl – plastic strain vector (EPPL)<br />

The plastic strains are assumed to develop instantaneously, that is, independent of time.<br />

The yield criterion<br />

where:<br />

{ σ}<br />

, κ)<br />

0<br />

F ( ≤<br />

(3-2)<br />

{σ} - stress vector<br />

κ - hardening parameter<br />

limit the stress domain. If the computed stress, using the elastic deformation matrix, exceeds the yield<br />

criteria (F>0), then plastic strain occurs. Plastic strains will computed by flow rule<br />

where:<br />

d pl<br />

ε<br />

∂Q<br />

= λ<br />

∂σ<br />

λ - plastic multiplier (which determines the amount of plastic straining)<br />

Q - plastic potential (which determines the direction of plastic straining)<br />

The plastic strains reduce the stress state so that it satisfies the yield criterion (F=0). By using associated<br />

flow rules, the plastic potential is equal the yield criterion and the vector of plastic strains is arranged perpendicularly<br />

to the yield surface.<br />

Q = F<br />

(3-4)<br />

By using non-associated flow rules<br />

Q ≠ F<br />

(3-5)<br />

effects that are known from experiments like dilatancy can be controlled more realistically.<br />

The hardening / softening function Ω(κ) describes the expansion and the reduction of the initial yield surface<br />

dependant on the load path, as well as the translation of the yield criterion in the stress domain. For<br />

the strain driven hardening/softening equations in <strong>multiPlas</strong> the scalar value κ serves as a weighting factor<br />

for plastic strain.<br />

pl pl<br />

dκ = dκ<br />

ε ) = dε<br />

eq<br />

7<br />

(3-3)<br />

( (3-6)<br />

The introduction of a separate softening function for each strength parameter made it possible to formulate<br />

an orthotropic softening model that is dependent from the failure mode. Existing relations, for example<br />

shear-tension interaction (mixed mode), were recognised.<br />

USER’S MANUAL, January, 2013

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