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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 />

propagates in a stable way converting a large part <strong>of</strong> <strong>the</strong> absorbed energy into<br />

plastic work.<br />

Both <strong>the</strong> material characterization <strong>and</strong> <strong>the</strong> specimen failure mechanisms pointed<br />

out <strong>the</strong> need <strong>of</strong> fracture mechanics tests in order to define <strong>the</strong> fracture toughness<br />

<strong>of</strong> <strong>the</strong> base material in <strong>the</strong> elastic-plastic regime. These tests, performed according<br />

to <strong>the</strong> ASTM E 813-89 code (1989), permitted <strong>the</strong> determination <strong>of</strong> <strong>the</strong> critical value<br />

J1c, viz. <strong>the</strong> change <strong>of</strong> <strong>the</strong> elastic-plastic work per unit crack extension at <strong>the</strong> onset<br />

<strong>of</strong> stable crack extension. Moreover, <strong>the</strong> critical value <strong>of</strong> <strong>the</strong> crack tip opening<br />

displacement (CTOD), in agreement with ASTM E 1290-93 code (1993) was<br />

measured. It provides a unique estimate <strong>of</strong> localized plastic strain. The samples<br />

used to determine J1c embodied a mechanical notch that was sharpened with a<br />

fatigue pre-crack induced by a constant amplitude sinusoidal loading. The multiple-<br />

specimen technique was adopted being <strong>the</strong> specimens drawn from <strong>the</strong> end plate<br />

normal to <strong>the</strong> weld bead. After fatigue pre-cracking, <strong>the</strong> specimens were subjected<br />

to a displacement controlled three-point bending test up to <strong>the</strong> crack extension. A<br />

value <strong>of</strong> J1c equal to 115 kJ/m 2 was obtained in accordance with literature data<br />

(SAC Background Reports, 1997). In addition, <strong>the</strong> critical value <strong>of</strong> <strong>the</strong> crack tip<br />

opening displacement (CTOD) was measured. In detail, <strong>the</strong> crack mouth opening<br />

displacement was detected through a displacement gauge, by means <strong>of</strong> quasi-<br />

static bending tests on a pre-cracked specimen. A value <strong>of</strong> 0.31 mm was obtained,<br />

showing a good correlation with <strong>the</strong> corresponding J1c value. As a matter <strong>of</strong> fact,<br />

<strong>the</strong> J1c value can be converted into <strong>the</strong> CTOD index through <strong>the</strong> following<br />

relationship:<br />

J = mσ CTOD<br />

( 3.1 )<br />

1c y<br />

where m is <strong>the</strong> so-called constraint factor. It is worthwhile to emphasize that CTOD<br />

values computed through <strong>the</strong> correlation in Equation (3.1) are approximate owing<br />

to <strong>the</strong> inherent variation <strong>of</strong> toughness properties <strong>of</strong> materials in building<br />

construction.<br />

3.4.3 Testing equipment <strong>and</strong> measuring apparatus<br />

All specimens were tested in a rigid reaction frame, illustrated in Figure 3.6. In<br />

detail, ITS specimens were connected directly to <strong>the</strong> rigid counter-beam <strong>of</strong> <strong>the</strong><br />

frame while a column stub was attached to <strong>the</strong> counter-beam in order to test CTS<br />

specimens as illustrated in Figure 3.6a. The loading arrangement relevant to CJ<br />

specimens is depicted in Figure 3.6b. The column is kept horizontal <strong>and</strong> hinged at<br />

both ends at <strong>the</strong> distance <strong>of</strong> 2000 mm while <strong>the</strong> horizontal loading is applied at <strong>the</strong><br />

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