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77<br />

and the inside of the damper cylinder housing. <strong>The</strong> damper has an inside diameter of 20.3 cm and a<br />

stroke of ±8 cm. <strong>The</strong> electromagnetic coils are wound in three sections on the piston, resulting in four<br />

effective valve regions as the fluid flows past the piston. <strong>The</strong> coils contain a total of about 1.5 km of<br />

wire. When wired in series, the total coil has an inductance L 0 = 6.6 H and a resistance R Q = 21.9 Q.<br />

<strong>The</strong> completed damper is approximately 1 m long and has a mass of 250 kg. <strong>The</strong> damper contains<br />

approximately 5 liters of MR fluid. <strong>The</strong> amount of fluid energized by the magnetic field at any given<br />

instant is approximately 90 cm 3 .<br />

Figure 13b shows the experimental setup at the <strong>University</strong> of Notre Dame for the large-scale 20-ton MR<br />

fluid damper. <strong>The</strong> damper was attached to a 7.5 cm thick plate that was grouted to a 2 m thick strong<br />

floor. <strong>The</strong> damper is driven by a 560 kN actuator configured with a 57 1pm servo-valve with a bandwidth<br />

of 30 Hz. A Schenck-Pegasus 5910 servo-hydraulic controller is employed in conjunction with a<br />

200 MPa, 340 1pm hydraulic pump. So that reliable tests of the dynamic performance could be obtained,<br />

particular care was taken to minimize compliance in the system.<br />

Analytical and experimental pseudo-static studies of the damper have been conducted at the Structural<br />

Dynamics and Control / <strong>Earthquake</strong> <strong>Engineering</strong> Laboratory at the <strong>University</strong> of Notre Dame. Figure<br />

14a shows the measured force-displacement loops under a commanded 5.4 cm/sec triangular displacement<br />

at the maximum magnetic field and no magnetic field (off state) respectively. At the maximum<br />

magnetic field, the output force of the damper is 201 kN, which is within 0.5% of the design specification<br />

of 200 kN. Moreover, the on/off range of the damper is well over the design specification of 10.<br />

Fig. 14b also shows the measured force-velocity relationship and its comparison with the results of the<br />

axisymmetric model and parallel plate model (Spencer et al 1999). Both analytical models compare<br />

well with the experimental results. <strong>The</strong> dynamic response of the damper to changes in the commanded<br />

force has also been shown to be excellent (Yang et al 2000; Yang 2001).<br />

Recently, Sunakoda et al (2000) have also presented encouraging results regarding design and construction<br />

of large scale MR dampers. More information regarding MR dampers and their application to<br />

civil engineering structures can be found at: hitpj/cee muc.edu/sstl/.<br />

Max Magnetic Reid (2A)<br />

No Magnetic Field iQA)<br />

Figure 14. (a) Measured force-displacement loops at 5.4 cm/sec; (b) Comparison of measured and<br />

predicted force-velocity behavior (Spencer et aL 1999)

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