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multiPlas - Dynardo GmbH

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This model guaranties a consistent dissipation of fracture energy during the softening process for different<br />

sizes of elements. The stress-strain lines available in <strong>multiPlas</strong> are shown in Fig. 3-13. Thereby, a linear<br />

elastic behaviour is assumed until the tensile strength is reached. After that, one of the following is<br />

assumed as consequence of tensile fracturing:<br />

** linear softening until the strain limit is reached εtr (mlaw = 0, 2) or<br />

** exponential softening (mlaw = 1)<br />

σ<br />

Fig. 3-13 Stress-strain relation in <strong>multiPlas</strong> (mlaw=0, 2; mlaw = 1)<br />

For the exponential softening model (mlaw = 1) one should assume<br />

G E<br />

h ≤ (3-24)<br />

f<br />

f<br />

2<br />

t<br />

Über h gemittelte Spannungs-Dehnungslinie<br />

f t<br />

f t/E<br />

(a)<br />

(b)<br />

"Snap-Back", wenn h groß<br />

ε tr<br />

h PR h<br />

for the length h in order to avoid the numerically unstable „snap-back“ phenomena. This is preferably<br />

achieved by choosing a proper mesh size. In <strong>multiPlas</strong>, the equivalent length will calculated automatically.<br />

(a)<br />

(b)<br />

h PR<br />

19<br />

USER’S MANUAL, January, 2013<br />

h<br />

ε

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