r - The Hong Kong Polytechnic University
r - The Hong Kong Polytechnic University
r - The Hong Kong Polytechnic University
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
columns were reinforced with three types of design details. One with 12-D19 main reinforcements was<br />
transversely reinforced with D13 perimeter hoops spaced 9 cm (volumetric confinement ratio ρ s = 0.012),<br />
corresponding to a case with sufficient transverse reinforcements. <strong>The</strong> other two with 18-D19 main<br />
reinforcements were transversely reinforced with D13 perimeter hoops spaced 9 cm and 18 cm, respectively. <strong>The</strong><br />
one with the transverse reinforcements spaced 18 cm was designed to represents a column with an insufficient<br />
volumetric confinement ratio (ρ s = 0.006) in order to investigate the ductility demand for a column allow to rock.<br />
<strong>The</strong> nominated material properties for these specimens are as follows: concrete compressive strength f c ’ =280<br />
kg/cm 2 ; yield strength of main reinforcements F y = 4200 kg/cm 2 ; yield strength of transverse reinforcements<br />
F yh =2800 kg/cm 2 . <strong>The</strong> test schedule is listed in Table 5, which also includes pseudo-dynamic loading test and<br />
quasi-static cyclic loading test.<br />
Test Results and Conclusions<br />
As mentioned previously, both series of rocking experiments include pseudo-dynamic test and cyclic loading<br />
test. However, only part of the cyclic loading test results will be presented in this paper due to the page limit of<br />
the paper. <strong>The</strong> test results of the first series of experiment are given Fig. 4. In this figure, (a) shows the lateral<br />
load versus the total lateral displacement curves and (b) shows the moment versus rotation curves at the column<br />
base. From these figures, it is evident that the hysteretic response for specimen B show a pattern of response<br />
behavior that is similar to that of specimen A, including exhibiting a sudden and significant loss of lateral<br />
resistance with low ductility under reversed cyclic deformation. However, the pinching effect in specimen B is<br />
not as serious as that in specimen A. If we further compare specimen A with specimen B at the same drift ratio<br />
of 5%, we can find that the rocking mechanism of specimen B resulted in an increase of lateral load resistance<br />
and a decrease of plastic deformation in the plastic hinge zone. This observation confirms the isolation effect of<br />
a rocking foundation. For the retrofitted specimen C, it demonstrates a nonlinear rocking behavior in Fig. (a)<br />
and that the seismic force that the pier sustained was limited to an almost constant value of 25 tonf. This means<br />
that specimen C was able to sustain large lateral displacement without significant strength degradation. <strong>The</strong><br />
plastic deformation of specimen C shown in the moment-rotation curve is also smaller than that of specimen B.<br />
30<br />
20<br />
Drift (%)<br />
-8 -6 -4 -2 0 2 4 6 8<br />
Specimen A<br />
(cyclic loading test)<br />
Drift (%)<br />
-8 -6 -4 -2 0 2 4 6 8<br />
30<br />
Specimen B<br />
20 (cyclic loading test)<br />
30<br />
20<br />
Drift (%)<br />
-8 -6 -4 -2 0 2 4 6 8<br />
Specimen C<br />
(cyclic loading test)<br />
Lateral force (tonf)<br />
10<br />
0<br />
-10<br />
Pull<br />
Push<br />
Lateral force (tonf)<br />
10<br />
0<br />
-10<br />
Pull<br />
Push<br />
Lateral force (tonf)<br />
10<br />
0<br />
-10<br />
Pull<br />
Push<br />
-20<br />
-20<br />
-20<br />
Moment (tonf-m)<br />
-30<br />
-30 -20 -10 0 10 20 30<br />
Lateral displacement (cm)<br />
100<br />
80<br />
60<br />
40<br />
20<br />
0<br />
-20<br />
-40<br />
-60<br />
-80<br />
Specimen A<br />
(cyclic loading test)<br />
Pull<br />
Push<br />
-100<br />
-0.08 -0.04 0 0.04 0.08<br />
Rotation (radians)<br />
Moment (tonf-m)<br />
-30<br />
-30 -20 -10 0 10 20 30<br />
Lateraldisplacement (cm)<br />
100<br />
80<br />
60<br />
40<br />
20<br />
0<br />
-20<br />
-40<br />
-60<br />
-80<br />
(a) Lateral force-displacement curves<br />
Specimen B<br />
(cyclic loading test)<br />
Pull<br />
Push<br />
-100<br />
-0.08 -0.04 0 0.04 0.08<br />
Rotation (radians)<br />
Moment (tonf-m)<br />
-30<br />
-30 -20 -10 0 10 20 30<br />
Lateral displacement (cm)<br />
100<br />
80<br />
60<br />
40<br />
20<br />
0<br />
-20<br />
-40<br />
-60<br />
-80<br />
Specimen C<br />
(cyclic loading test)<br />
Pull<br />
Push<br />
-100<br />
-0.08 -0.04 0 0.04 0.08<br />
Rotation (radians)<br />
(b) Moment-rotation curves<br />
Figure 4 Experimental results for the cyclic loading test of specimens A, B and C<br />
In theory, if the foundation of a pier is allowed to rock with the uplift, the foundation lifts off the ground once its<br />
moment of resistance provided by gravity is overcome. Thus, the base moment can be limited to the value<br />
required to produce uplift against the restraining forces due to gravity. <strong>The</strong> base moment limitation will then<br />
possibly reduce the inelastic deformation of the pier at the plastic hinge zone. <strong>The</strong>se experiments showed that<br />
there was a decrease of plastic deformation at the plastic hinge of a column as a result of the energy dissipation<br />
of the inelastic rocking mechanism of the footing. However, this effect is not very significant for the<br />
un-retrofitted case of specimen B. This is because before the base moment of the foundation could reach its limit<br />
value, the column yielded and the strength degraded earlier due to its inadequate lap-splicing of the main<br />
reinforcements and poor transverse confinement. Because the column yielded before the isolation effect of<br />
-111-