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iter structural design criteria for in-vessel components (sdc-ic)

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ITER G 74 MA 8 01-05-28 W0.2<br />

p<br />

Plast<strong>ic</strong> stra<strong>in</strong> eij is calculated <strong>in</strong>crementally by us<strong>in</strong>g the flow rule given <strong>in</strong> ICÊ3024.2.3. In<br />

the case of a material wh<strong>ic</strong>h can stra<strong>in</strong> harden, the plast<strong>ic</strong> stra<strong>in</strong> modifies the yield cr<strong>iter</strong>ion.<br />

This modif<strong>ic</strong>ation is determ<strong>in</strong>ed by means of the harden<strong>in</strong>g rule given <strong>in</strong> ICÊ3024.2.4.<br />

BÊ3024.2.3 Flow rule<br />

p<br />

The flow rule provides the <strong>in</strong>cremental plast<strong>ic</strong> stra<strong>in</strong> de ij <strong>for</strong> a given <strong>in</strong>cremental stress dsij.<br />

The <strong>in</strong>cremental plast<strong>ic</strong> stra<strong>in</strong> at any po<strong>in</strong>t can be obta<strong>in</strong>ed by us<strong>in</strong>g the follow<strong>in</strong>g steps.<br />

1) At the start of a step, the current stress, stra<strong>in</strong>, and plast<strong>ic</strong> stra<strong>in</strong> at a given po<strong>in</strong>t<br />

is known. By def<strong>in</strong>ition, the current stress is on the current yield surface wh<strong>ic</strong>h<br />

is known:<br />

2<br />

3<br />

* * 2<br />

f( s©, ij s ) s© ij s© ij s<br />

where<br />

= - ( ) =<br />

s'ij is the deviator<strong>ic</strong> stress.<br />

SDC-IC, Appendix B. Guidel<strong>in</strong>es <strong>for</strong> Analysis page 32<br />

0,<br />

2) For a given stress <strong>in</strong>crement dsij , the deviator<strong>ic</strong> stress <strong>in</strong>crement ds'ij can be<br />

calculated. The po<strong>in</strong>t under consideration will undergo further plast<strong>ic</strong><br />

de<strong>for</strong>mation if s'ij ds'ij > 0. The stress <strong>in</strong>crement will cause an elast<strong>ic</strong> stra<strong>in</strong><br />

<strong>in</strong>crement only if s'ij ds'ij £ 0.<br />

3) If further plast<strong>ic</strong> de<strong>for</strong>mation occurs, the plast<strong>ic</strong> stra<strong>in</strong> <strong>in</strong>crement is determ<strong>in</strong>ed<br />

by the normality rule (Reuss equations)<br />

de<br />

p<br />

ij<br />

f<br />

= dl = s© ij dl<br />

s©<br />

ij<br />

.<br />

Def<strong>in</strong><strong>in</strong>g an equivalent plast<strong>ic</strong> stra<strong>in</strong> <strong>in</strong>crement by<br />

p<br />

de =<br />

p p<br />

deijdeij 2<br />

,<br />

3<br />

wh<strong>ic</strong>h can be written <strong>in</strong> an expanded <strong>for</strong>m as<br />

( ) + ( - ) + ( - )<br />

2<br />

de =<br />

ì<br />

2<br />

2<br />

í de11 - de22 de22 de33 de de<br />

3 î<br />

12<br />

p p p<br />

+<br />

æ 2 2 2<br />

( de ) + ( de ) + ( de<br />

ö ü<br />

6<br />

è 12 23 31)<br />

ø ý<br />

þ<br />

p p p p p p p 2<br />

33 11<br />

dl can be solved as<br />

dl<br />

d p<br />

3 e<br />

= *<br />

2 s ,<br />

and the <strong>in</strong>cremental plast<strong>ic</strong> stra<strong>in</strong> <strong>components</strong> are then given by :<br />

,

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