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r - The Hong Kong Polytechnic University

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vertical stiffness of primary suspension system k s = 1.4 MN/m, vertical damping of primary suspension system<br />

d p = 0.03MN-s/m, and characteristic length α = 0.745 m. FRA track class 1 is adopted in generating the<br />

artificial irregularities profile u w/r (y) for the rails, which corresponds to the poorest rail quality. <strong>The</strong> lower and<br />

upper bounds of the wavenumbers [k yl , k yu ] defined in the single sided PSD are chosen to be 0.1 and 15 rad/m,<br />

respectively, with n = 40 intervals. <strong>The</strong> corresponding wavelengths of rail unevenness considered range from L i<br />

= 0.42 to 62.8 m. By assuming the train speed to be c = 50 m/s, the major frequencies involved in the rail<br />

irregularities range from 7 to 119 Hz. Thus the analysis frequency range selected is from 0 to 150 Hz.<br />

Table 2. Material Properties.<br />

Young’s modulus<br />

E (MPa)<br />

Poisson’s ratio<br />

υ<br />

Mass density<br />

ρ (kg/m 3 )<br />

Damping ratio<br />

β<br />

Material<br />

Concrete tunnel lining 35,000 0.25 2,500 0.02<br />

Concrete slab 28,500 0.2 2,500 0.02<br />

Elastic Foundation 0.5 0.25 150 0.1<br />

Fill material 116.6 0.341 1,900 0.05<br />

Silty clay 289 0.313 2,023 0.04<br />

Gravel and pebble 704 0.223 1,963 0.03<br />

For train speed equal to c = 50 m/s, the responses computed for X = 0 m and X = 50 m on the ground with and<br />

without an elastic foundation supporting the concrete slab track were plotted in Figure 8, with parts (a) to (c)<br />

showing the time histories of displacement, velocity and acceleration, respectively. As indicated by Figure 8(a),<br />

there exists a localized quasi-static displacement combined with distinct fluctuating vibrations for the case<br />

without floating slab track. This is mainly caused by the moving tributary weight of the train, quasi-static in<br />

nature, while the fluctuating vibrations are induced by rail irregularities. For the case with floating slab track,<br />

although the fluctuating vibrations with high frequencies are reduced by the elastic foundation, the localized<br />

displacements and the fluctuating vibration with low frequencies increase.<br />

(a) Displacement<br />

(b) Velocity<br />

(c) Acceleration<br />

Figure 8 Effect of elastic foundation on the ground response caused by a moving train over uneven rails: (a)<br />

displacement, (b) velocity, (c) acceleration<br />

<strong>The</strong> isolation effect of the floating slab track is clearer from the velocity and acceleration responses in Figures<br />

8(b) and (c), as the high-frequency components have been suppressed. Such an observation is also confirmed by<br />

the spectra shown in Figures 9(a) and (b) for the responses at X = 0 m and 50 m, respectively. <strong>The</strong> isolation<br />

effect of elastic foundations is generally poor for vibrations at lower frequencies, but effective for higher<br />

frequencies. Because the acceleration has a frequency content covering mostly higher frequencies, the isolation<br />

effect of floating slab track is generally significant. In contrast, the frequency content of the displacement<br />

response is mostly localized on the low-frequency region, which makes the effect of isolation not so effective.<br />

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