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

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3. SEISMIC BEHAVIOUR OF BOLTED END PLATE BEAM-TO-COLUMN STEEL JOINTS<br />

56<br />

M col,t<br />

Vcol,t<br />

f<br />

f<br />

c<br />

N<br />

N<br />

col,b<br />

V<br />

col,t<br />

col,b<br />

M col,b<br />

b<br />

V beam<br />

M beam<br />

N beam<br />

Figure 3.8. Definition <strong>of</strong> rotations for a Complete<br />

Joint<br />

3.4.4 Testing procedure<br />

Predefined representative displacement histories are usually applied in order to<br />

characterize <strong>the</strong> <strong>behaviour</strong> <strong>of</strong> specimens under hysteretic loading. The problem <strong>of</strong><br />

<strong>the</strong> displacement pattern arises especially under <strong>seismic</strong> loading, as unique fatigue<br />

relationships are strictly valid only for constant-amplitude displacement reversals.<br />

Real structures, however, seldom conform to this ideal as <strong>the</strong>y can be subjected to<br />

multitude <strong>of</strong> displacement patterns <strong>of</strong> varying degrees <strong>of</strong> complexity. In <strong>the</strong>se<br />

instances, probability-density curves able to characterize r<strong>and</strong>om-amplitude<br />

displacements should be employed. In order to reduce <strong>the</strong> problem complexity, a<br />

heuristic approach is adopted in this study, applying to <strong>the</strong> specimens several<br />

displacement histories lying between <strong>the</strong> extremes <strong>of</strong> constant-amplitude <strong>and</strong><br />

r<strong>and</strong>om-amplitude displacement reversals.<br />

In order to define conveniently displacement patterns, a conventional elastic limit<br />

+ +<br />

state characterized by <strong>the</strong> displacement ey <strong>and</strong> <strong>the</strong> corresponding force Fy can be<br />

defined on <strong>the</strong> first part <strong>of</strong> each non-linear response envelope obtained from<br />

monotonic tests as depicted in Figure 3.9, schematically. The tri-linear<br />

approximation <strong>of</strong> each curve, is determined on <strong>the</strong> basis <strong>of</strong> best-fitting <strong>and</strong> <strong>of</strong> <strong>the</strong><br />

equivalence <strong>of</strong> <strong>the</strong> dissipated energy between <strong>the</strong> actual non-linear response <strong>and</strong><br />

+ +<br />

<strong>the</strong> idealized tri-linear approximation up to (emax , Fmax ). Then, <strong>the</strong> linear elastic<br />

+ +<br />

response with slope Ke <strong>and</strong> <strong>the</strong> linear strain-hardening response with slope Kh

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