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Seismic Design of Tunnels - Parsons Brinckerhoff

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4.0 OVALING EFFECT ON CIRCULAR TUNNELS<br />

The primary purpose <strong>of</strong> this chapter is to provide methods for quantifying the seismic<br />

ovaling effect on circular tunnel linings. The conventionally used simplified free-field<br />

deformation method, discussed first, ignores the soil-structure interaction effects.<br />

Therefore its use, as demonstrated by two examples, is limited to certain conditions.<br />

A refined method is then presented that is equally simple but capable <strong>of</strong> eliminating the<br />

drawbacks associated with the free-field deformation method. This refined method — built<br />

from a theory that is familiar to most mining/underground engineers — considers the soilstructure<br />

interaction effects. Based on this method, a series <strong>of</strong> design charts are developed<br />

to facilitate the design process. The results are further validated through numerical analyses.<br />

4.1 Ovaling Effect<br />

As defined in Chapter 3, ovaling <strong>of</strong> a circular tunnel lining is primarily caused by<br />

seismic waves propagating in planes perpendicular to the tunnel axis (see Figure 2).<br />

Usually, it is the vertically propagating shear waves that produce the most critical ovaling<br />

distortion <strong>of</strong> the lining. The results are cycles <strong>of</strong> additional stress concentrations with<br />

alternating compressive and tensile stresses in the tunnel lining. These dynamic stresses<br />

are superimposed on the existing static state <strong>of</strong> stress in the lining. Several critical modes<br />

may result (Owen and Scholl, 1981):<br />

• Compressive dynamic stresses added to the compressive static stresses may exceed<br />

the compressive capacity <strong>of</strong> the lining locally.<br />

• Tensile dynamic stresses subtracted from the compressive static stresses reduce the<br />

lining’s moment capacity, and sometimes the resulting stresses may be tensile.<br />

4.2 Free-Field Shear Deformations<br />

As discussed in Chapter 3, the shear distortion <strong>of</strong> ground caused by vertically<br />

propagating shear waves is probably the most critical and predominant mode <strong>of</strong> seismic<br />

motions in many cases. It causes a circular tunnel to oval and a rectangular underground<br />

structure to rack (sideways motion), as shown in Figure 3. Analytical procedures by<br />

numerical methods are <strong>of</strong>ten required to arrive at a reasonable estimate <strong>of</strong> the free-field<br />

shear distortion, particularly for a soil site with variable stratigraphy. Many computer<br />

codes with variable degree <strong>of</strong> sophistication are available (e.g., SHAKE, 1972; FLUSH,<br />

1975; and LINOS, 1991).<br />

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