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Analysis and modelling of the seismic behaviour of high ... - Ingegneria

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4. SEISMIC RESPONSE OF PARTIAL-STRENGTH COMPOSITE JOINTS<br />

where Fb <strong>and</strong> dn are, respectively, <strong>the</strong> base shear force <strong>and</strong> <strong>the</strong> control node<br />

displacement <strong>of</strong> <strong>the</strong> MDoF system.<br />

ii. Definition <strong>of</strong> <strong>the</strong> yield force F *<br />

y, which also represents <strong>the</strong> ultimate strength <strong>of</strong><br />

<strong>the</strong> idealized system; it is equal to <strong>the</strong> base shear force at <strong>the</strong> formation <strong>of</strong> <strong>the</strong><br />

plastic mechanism. The initial stiffness <strong>of</strong> <strong>the</strong> idealized system is determined in<br />

such a way that <strong>the</strong> areas under <strong>the</strong> actual <strong>and</strong> <strong>the</strong> idealized force–deformation<br />

curves are equal (see Figure 4.47).<br />

Figure 4.47. Determination <strong>of</strong> <strong>the</strong> idealized elasto-perfectly<br />

plastic force-displacement relationship (EC8, 2002)<br />

Based on this assumption, <strong>the</strong> yield displacement <strong>of</strong> <strong>the</strong> idealized SDoF<br />

system d *<br />

y is given by:<br />

*<br />

y<br />

*<br />

* Em<br />

= 2 d m − *<br />

F<br />

d ( 4.32 )<br />

y<br />

where E *<br />

m is <strong>the</strong> actual deformation energy up to <strong>the</strong> formation <strong>of</strong> <strong>the</strong> plastic<br />

mechanism.<br />

iii. Determination <strong>of</strong> <strong>the</strong> period T * <strong>of</strong> <strong>the</strong> idealized equivalent SDOF system,<br />

determined by:<br />

*<br />

T 2π<br />

m d<br />

* *<br />

y<br />

*<br />

y<br />

= ( 4.33 )<br />

F<br />

153

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