2023
DOI: 10.1002/eqe.3850
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Effect of a symmetric V‐shaped canyon on the seismic response of an adjacent building under oblique incident SH waves

Abstract: To elucidate whether an irregular topography affects the seismic response of nearby structures, an analytical solution to the dynamic interaction between a symmetric V-shaped canyon and an adjacent building under the incidence of SH waves is proposed by using the wave function expansion method. The dynamic canyon-soil-structure interaction is decomposed into two problems of scattering and radiation. The building is idealized as a shear wall supported by a semicircular rigid foundation. The analytical solution … Show more

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Cited by 11 publications
(10 citation statements)
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“…According to Zhang et al 18 . and with aid of Equation (), the free wave u f in various coordinate systems ( r j , θ j ) for j = 1, 2, 3 can be expressed in a unified form as uf()rj,θjbadbreak=n=0Un,jJn()krjcos()nθj$$\begin{equation}{u^f}\left( {{r_j},{\theta _j}} \right) = \sum_{n = 0}^\infty {{U_{n,j}}} {J_n}\left( {k{r_j}} \right)\cos \left( {n{\theta _j}} \right)\end{equation}$$where J n (•) is the Bessel function of the first kind with order n and Un,jbadbreak={2()1nεncosnαexpikD12cosαj=12()1nεncosnαj=22()1nεncosnαexpikD23cosαj=3$$\begin{equation}{U_{n,j}} = \left\{ { \def\eqcellsep{&}\begin{array}{@{}*{2}{c}@{}} {2{{\left( { - 1} \right)}^n}{\varepsilon _n}\cos \left( {n\alpha } \right)\exp \left( {ik{D_{12}}\cos \alpha } \right)}&{j = 1}\\[4pt] {2{{\left( { - 1} \right)}^n}{\varepsilon _n}\cos \left( {n\alpha } \right)}&{j = 2}\\[4pt] {2{{\left( { - 1} \right)}^n}{\varepsilon _n}\cos \left( {n\alpha } \right)\exp \left( { - ik{D_{23}}\cos \alpha } \right)}&{j = 3} \end{array} } \right.\end{equation}$$with ε n being the Newman factor ( ε n = 1, n = 0; ε n = 2, n > 0).…”
Section: Model and Mathematical Formulationmentioning
confidence: 99%
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“…According to Zhang et al 18 . and with aid of Equation (), the free wave u f in various coordinate systems ( r j , θ j ) for j = 1, 2, 3 can be expressed in a unified form as uf()rj,θjbadbreak=n=0Un,jJn()krjcos()nθj$$\begin{equation}{u^f}\left( {{r_j},{\theta _j}} \right) = \sum_{n = 0}^\infty {{U_{n,j}}} {J_n}\left( {k{r_j}} \right)\cos \left( {n{\theta _j}} \right)\end{equation}$$where J n (•) is the Bessel function of the first kind with order n and Un,jbadbreak={2()1nεncosnαexpikD12cosαj=12()1nεncosnαj=22()1nεncosnαexpikD23cosαj=3$$\begin{equation}{U_{n,j}} = \left\{ { \def\eqcellsep{&}\begin{array}{@{}*{2}{c}@{}} {2{{\left( { - 1} \right)}^n}{\varepsilon _n}\cos \left( {n\alpha } \right)\exp \left( {ik{D_{12}}\cos \alpha } \right)}&{j = 1}\\[4pt] {2{{\left( { - 1} \right)}^n}{\varepsilon _n}\cos \left( {n\alpha } \right)}&{j = 2}\\[4pt] {2{{\left( { - 1} \right)}^n}{\varepsilon _n}\cos \left( {n\alpha } \right)\exp \left( { - ik{D_{23}}\cos \alpha } \right)}&{j = 3} \end{array} } \right.\end{equation}$$with ε n being the Newman factor ( ε n = 1, n = 0; ε n = 2, n > 0).…”
Section: Model and Mathematical Formulationmentioning
confidence: 99%
“…Based on the above problem decomposition strategy similar to Zhang et al., 18 once the Problems I, II and III are solved, the total scattering wavefields us 1, us 2 and us 3 in the outer region and the total wavefield u in in the inner region can be obtained by the following relations: umsbadbreak=um,Isgoodbreak+um,IIsΔ1goodbreak+um,IIIsΔ3,mgoodbreak=1,2,3$$\begin{equation}u_m^s = u_{m,I}^s + u_{m,II}^s{\Delta _1} + u_{m,III}^s{\Delta _3},m = 1,2,3\end{equation}$$ uinbadbreak=uIingoodbreak+uIIinΔ1goodbreak+uIIIinΔ3$$\begin{equation}{u^{in}} = u_I^{in} + u_{II}^{in}{\Delta _1} + u_{III}^{in}{\Delta _3}\end{equation}$$…”
Section: Model and Mathematical Formulationmentioning
confidence: 99%
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