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219<br />

3 360 Deg. Fault Normal (Jan. 17, 1994), peak acceleration: 0.59 g (100%); (4) Sylmar Channel 1 90 Deg<br />

Fault Parallel (Jan. 17, 1994), peak acceleration: 0.461 g (80%); (5) Sylmar Channel 3 360 Deg. Fault<br />

Normal (Jan. 17, 1994), peak acceleration: 0,84 g (100%); (6) Kobe NS (Jan. 17, 1995), peak acceleration:<br />

0816 g (100%); (7) Kobe EW (Jan. 17, 1995), peak acceleration: 0.62 g (100%). <strong>The</strong> records are time<br />

scaled by a factor of 2.236 to satisfy similitude requirements. <strong>The</strong> peak accelerations are scaled from the<br />

original recorded values. Results are presented in Table 1 to Table 3. Table 1 shows peak values of relative<br />

base displacement and normalized peak shear force at the isolation level (total of friction force, MR damper<br />

force, and spring force normalized by total weight). Table 2 shows the peak values of first floor and second<br />

floor inter-story drifts. Table 3 shows the peak values of first floor and second floor accelerations.<br />

In Tables 1 to 3 in case of Sylmar, Newhall, and Kobe earthquakes, the relative base displacement<br />

reductions range from 5 to 40 % in the passive high damping (4 volt) case when compared to the passive<br />

low damping (0 volt) case. This occurs due to the increase in energy dissipation in high damping case, with<br />

nearly 5 to 30 % increase in the peak total force at the isolation level when compared to the low damping case.<br />

<strong>The</strong> semiactive controlled case gives an additional 5 to 15 % reduction in the base displacement response<br />

over the passive high damping (4 volt) case. <strong>The</strong> controlled case also reduces or maintains the same level<br />

of total force at the isolation level when compared to the high damping case. Hence, the controlled case<br />

reduces the base displacement further, when compared to 0 volt and 4 volt cases, with no further increase<br />

in force as compared to 4 volt case. <strong>The</strong> energy dissipation occurs more efficiently in the controlled case<br />

revealing the potential of smart damping. In most cases the interstory drifts in the controlled case are the<br />

smaller than the passive high damping case—which indicates the effectiveness of the smart isolation system,<br />

<strong>The</strong> accelerations in the controlled case remain bounded by the high and low damping cases. As evident<br />

from Table 1 in case of Sylmar 360 earthquake the peak relative base displacement, the largest amongst all<br />

earthquakes, is reduced by 42% in the passive high damping (4 volt) case when compared to the passive low<br />

damping (0 volt) case. <strong>The</strong> passive high damping (4 volt) case also reduces the total force at isolation level<br />

by 4% when compared to the passive low damping (0 volt) case. <strong>The</strong> controlled case gives additional 7%<br />

reduction in the base displacement response over the passive high damping (4 volt) case; the control case<br />

also maintains the same level of total force at the isolation level as compared to that of the passive high<br />

damping case. Thus based on the results in Tables 1, 2 and 3 it can be concluded that the controlled case<br />

reduces the base displacement further and maintains the total force at the isolation level within bounds in<br />

most earthquakes-the one exception being El Centro. In addition the controlled case maintains the interstory<br />

drifts and acceleration response of the two-story model within bounds. Thus the newly developed<br />

Lyapunov based control algorithm and the smart isolation system with MR damper is effective in reducing<br />

the base displacements, without further increases in the total force at the isolation level, interstory drifts<br />

and accelerations.<br />

Table 1 Peak Relative Base Displacement and Normalized Peak Shear Force at the Isolation Level of the<br />

Two-story Smart Sliding Isolated Structure<br />

<strong>Earthquake</strong> Rel. Base Disp.(cm) Force at Isolation Level/W<br />

El Centro(100%)<br />

Sylmar 90 (80%)<br />

Sylmar 90(100%)<br />

Sylmar 360(105%)<br />

Newhall 90(100%)<br />

Newhall 360(100%)<br />

Kobe NS(80%)<br />

Kobe NS(100%)<br />

Kobe EW<br />

0 Volt<br />

0.938<br />

2.293<br />

3.00<br />

5.48<br />

1.815<br />

3.867<br />

2.511<br />

3.362<br />

2.578<br />

4 Volt<br />

0.85<br />

1.649<br />

2.15<br />

3.183<br />

1.614<br />

3.373<br />

2.45<br />

2.825<br />

2.24<br />

Control<br />

0.77<br />

1.484<br />

2.1<br />

3.02<br />

1.276<br />

3.294<br />

2.105<br />

2.543<br />

2.22<br />

0 Volt<br />

0.16<br />

0.224<br />

0.254<br />

0.354<br />

0.21<br />

0.293<br />

0.204<br />

0.235<br />

0.236<br />

4 Volt<br />

0.244<br />

L 0.263<br />

0.292<br />

0.343<br />

0.28<br />

0.349<br />

0.29<br />

0.312<br />

0.305<br />

Control<br />

0.243<br />

0.26<br />

0.279<br />

0.34<br />

0.261<br />

0.29<br />

0.28<br />

0.3<br />

0.278<br />

Comparison with Experimental Results<br />

Comparison of analytical and experimental results are presented in Table 4 for three earthquakes: (1)

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