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Seismic Design of Tunnels - Parsons Brinckerhoff

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- In the JSCE (Japanese Society <strong>of</strong> Civil Engineers) Specifications for Earthquake<br />

Resistant <strong>Design</strong> <strong>of</strong> Submerged <strong>Tunnels</strong>, the values <strong>of</strong> wavelength that will<br />

maximize Equations 3-1, 3-3 and 3-4 are determined and substituted back into<br />

each respective equation to yield the maximum sectional forces.<br />

- St. John and Zahran (1987) suggested a maximization scheme that is similar to<br />

the Japanese approach except that the spring coefficients (K a or K t ) are assumed<br />

to be functions <strong>of</strong> wavelength, L, in the maximization process.<br />

Both <strong>of</strong> these approaches assume that the free-field ground displacement response<br />

amplitude, D, is independent <strong>of</strong> the wavelength. This assumption sometimes may<br />

lead to very conservative results, as the ground displacement response amplitude<br />

generally decreases with the wavelength. It is, therefore, the author’s view that<br />

Equations 3-1 through 3-4 presented in this section will provide a practical and<br />

adequate assessment, provided that the values (or the ranges <strong>of</strong> the values) <strong>of</strong> L, D,<br />

and K t (or K a ) can be reasonably estimated.<br />

A reasonable estimate <strong>of</strong> the wavelength can be obtained by<br />

L = T C s<br />

(Eq. 3-5)<br />

where T is the predominant natural period <strong>of</strong> the shear wave traveling in the soil<br />

deposit in which the tunnel is built, and C s is the shear wave propagation velocity<br />

within the soil deposit.<br />

Often, T can also be represented by the natural period <strong>of</strong> the site. Dobry, Oweis and<br />

Urzua (1976) presented some procedures for estimating the natural period <strong>of</strong> a linear<br />

or equivalent linear model <strong>of</strong> a soil site.<br />

• The ground displacement response amplitude, D, should be derived based on sitespecific<br />

subsurface conditions by earthquake engineers. The displacement<br />

amplitude represents the spatial variations <strong>of</strong> ground motions along a horizontal<br />

alignment. Generally, the displacement amplitude increases as the wavelength, L,<br />

increases. For example, the displacement spectrum chart prepared by Housner<br />

(SFBARTD, 1960) for the SF BART project was expressed by D = 4.9 x 10 -6 L 1.4 ,<br />

where the units <strong>of</strong> D and L are in feet. This spectrum is intended for tunnel tubes in<br />

s<strong>of</strong>t San Francisco Bay muds and was derived for a magnitude 8.2 earthquake on the<br />

San Andreas fault. The equation shows clearly that:<br />

- The displacement amplitude increases with the wavelength.<br />

- For any reasonably given wavelength, the corresponding ground displacement<br />

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