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