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Earthquake Engineering Research - HKU Libraries - The University ...

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553<br />

the laboratory and (2) that imposed during numerical differentiation due to time stepping.<br />

High frequencies introduced during testing occurred because the cameras were mounted on the<br />

reaction floor surround the shake table and the shake table itself induces some motion into the<br />

surrounding floor during earthquake simulation. <strong>The</strong> magnitude of this noise was consistently observed<br />

to be small and outside of the frequencies of interest (> 50 Hz), thus it could easily be filtered in the<br />

frequency domain using a 4 th Order low-pass Butterworth filter.<br />

Double numerical differentiation also creates noise in acceleration traces. In this case, a 10 th Order<br />

low-pass Butterworth filter was applied after numerical differentiation to remove introduced high<br />

frequency noise. Low pass filters of comparable details were also applied to the conventional<br />

accelerometer measurements.<br />

Figure 4 shows a comparison of<br />

acceleration and velocity time<br />

Iristories (absolute) measured from<br />

the 5 th floor (roof level) of the<br />

structure during the Mexico City<br />

event with the roof isolation system<br />

engaged. Accelerations are<br />

compared between the double<br />

differentiated vision-system<br />

positional data and the conventional<br />

accelerometers. Velocities are<br />

compared between the single<br />

differentiated vision system data<br />

and integrated accelerometer<br />

measurements. <strong>The</strong>se comparisons<br />

are very promising, with differences<br />

in maximum acceleration of 0.06g<br />

and differences in maximum<br />

velocity of 6 cm/second observed.<br />

Analysis of other floor levels and<br />

the different experiments showed<br />

that this was the largest difference<br />

between the two systems. However,<br />

_^<br />

o<br />

to<br />

Time (seconds)<br />

FIGURE 4. Comparison of velocity (a) and acceleration (b) time<br />

histories (absolute) at the roof level - Mexico City input motion<br />

with the roof isolation system engaged.<br />

it should be noted that selection of cut-off frequencies during the data processing was an important step<br />

in the evaluation of each case due to the different frequencies induced by the earthquake motions.<br />

SUMMARY<br />

A vision-based motion tracking system was evaluated for its accuracy in monitoring the seismic<br />

demands induced in a 5-story scale moment resisting frame structure. Reasonable comparison between<br />

time-varying positional responses was observed when comparing the vision system with conventional<br />

LVDT measurements. Although the system was calibrated statically to within a 1 mm displacement,<br />

the average difference in maximum displacements was observed as 1.4 mm. Signal processing and<br />

numerical differentiation of the positional data was required for 'calculating acceleration and velocity<br />

time histories from the vision-based (positional) measurements. Two aspects of high frequency noise

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