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ON THE EFFECTS OF CIRCULAR BOLT PATTERNS ON THE ...

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The analyses were conducted by applying the increasing cyclic variable amplitude displacement at<br />

the tip of the beam. The cyclic displacement amplitude followed the loading protocol in the AISC Seismic<br />

Provisions [73], which is identical to the SAC loading protocol, and FEMA [74]. The loading protocol<br />

composed of the following steps was incorporated in ABAQUS:<br />

Step 1: 6 cycles with peak drift angle of 0.00375 rad<br />

Step 2: 6 cycles with peak drift angle of 0.005 rad<br />

Step 3: 6 cycles with peak drift angle of 0.0075 rad<br />

Step 4: 4 cycles with peak drift angle of 0.01 rad<br />

Step 5: 2 cycles with peak drift angle of 0.015 rad<br />

Step 6: 2 cycles with peak drift angle of 0.02 rad<br />

Step 7: 2 cycles with peak drift angle of 0.03 rad<br />

Step 8 and further steps will be repeated with the drift angle of 0.01 rad for each 2 cycles until the<br />

beam or connection zone reaches inelastic mode.<br />

The loading protocol is shown in<br />

Figure 5-4. The tip displacement corresponding to a story drift ratio of 0.01 rad was 2.4 in. (60 mm).<br />

A rigid part (un-deformable mesh region) was attached to the tip of the beam to simulate a rigid beam<br />

end-cap which distribute the load caused by the cyclic displacement control evenly at the tip of the beam<br />

(Figure 5-3). Similarly, two rigid parts was attached at both ends of the column to distribute the support<br />

reaction forces evenly at the tip of the column (see Figure 5-3).<br />

72

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