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Seismic Design of Tunnels - Parsons Brinckerhoff

Seismic Design of Tunnels - Parsons Brinckerhoff

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where<br />

g s = angular distortion <strong>of</strong> the structure<br />

D s = lateral racking deformation <strong>of</strong> the structure<br />

g free-field = shear distortion/strain <strong>of</strong> the free-field<br />

D free-field = lateral shear deformation <strong>of</strong> the free-field<br />

The racking coefficients, R, obtained from the analyses are presented in the last<br />

column <strong>of</strong> Table 4 for all 25 cases.<br />

Note that the total structural deformation obtained from the finite element analyses<br />

contains a rigid body rotational movement, which causes no distortion to the cross-section<br />

<strong>of</strong> the structure. Therefore, this portion <strong>of</strong> the movement is excluded in the calculation <strong>of</strong><br />

the structure racking deformation.<br />

Effect <strong>of</strong> Relative Stiffness. As expected, results <strong>of</strong> the analyses indicate that the relative<br />

stiffness between the soil medium and the structure has the most significant influence on<br />

the structure response. This is demonstrated in Figure 33, where the structure racking<br />

coefficients, R, are plotted against the flexibility ratios, F.<br />

• When the flexibility ratio approaches zero, representing a perfectly rigid structure, the<br />

structure does not rack regardless <strong>of</strong> the distortion <strong>of</strong> the ground in the free-field. The<br />

normalized structure distortion (i.e., R) increases with the increasing flexibility ratio. At<br />

F=1, the structure is considered to have the same stiffness as the ground and<br />

therefore is subjected to a racking distortion that is comparable in magnitude to the<br />

ground distortion in the free field (i.e., Rª1).<br />

• With a flexibility ratio greater than 1.0, the structure becomes flexible relative to the<br />

ground and the racking distortion will be magnified in comparison to the shear<br />

distortion experienced by the ground in the free field. This latter phenomenon is not<br />

caused by the effect <strong>of</strong> dynamic amplification. Rather, it is primarily attributable to the<br />

fact that the ground surrounding the structure has a cavity in it (i.e., a perforated<br />

ground). A perforated ground, compared to the non-perforated ground in the free<br />

field, has a lower stiffness in resisting shear distortion and thus will distort more than<br />

will the non-perforated ground.<br />

An interesting presentation <strong>of</strong> these data for rectangular structures is shown in Figures<br />

34 and 35, where the closed-form solutions obtained for the normalized circular lining<br />

deflections (Figure 15 in Chapter 4) are superimposed. Note that the definitions <strong>of</strong><br />

flexibility ratio, F, are different.<br />

• For circular tunnels, Equation 4-6 is used.<br />

• For rectangular tunnels, Equation 5-5, 5-6 or 5-7, as appropriate, is used.<br />

114

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