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Trường DCGiá trị Ngôn ngữ
dc.contributor.authorZhou, Xiaojie-
dc.contributor.authorLiang, Qinghua-
dc.contributor.authorLiu, Zhongxian-
dc.contributor.authorHe, Ying-
dc.date.accessioned2020-05-30T07:04:29Z-
dc.date.available2020-05-30T07:04:29Z-
dc.date.issued2019-
dc.identifier.issn1687-8086-
dc.identifier.issn1687-8094 (eISSN)-
dc.identifier.otherBBKH1281-
dc.identifier.urihttp://thuvienso.vanlanguni.edu.vn/handle/Vanlang_TV/18559-
dc.description"Hindawi; Advances in Civil Engineering; Volume 2019, Article ID 1025483, 14 pages; https://doi.org/10.1155/2019/1025483"vi
dc.description.abstractA viscous-slip interface model is proposed to simulate the contact state between a tunnel lining structure and the surrounding rock. The boundary integral equation method is adopted to solve the scattering of the plane SV wave by a tunnel lining in an elastic half-space. We place special emphasis on the dynamic stress concentration of the lining and the amplification effect on the surface displacement near the tunnel. Scattered waves in the lining and half-space are constructed using the fictitious wave sources close to the lining surfaces based on Green’s functions of cylindrical expansion and the shear wave source. The magnitudes of the fictitious wave sources are determined by viscous-slip boundary conditions, and then the total response is obtained by superposition of the free and scattered fields. The slip stiffness and viscosity coefficients at the lining-surrounding rock interface have a significant influence on the dynamic stress distribution and the nearby surface displacement response in the tunnel lining. Their influence is controlled by the incident wave frequency and angle. The hoop stress increases gradually in the inner wall of the lining as sliding stiffness increases under a low-frequency incident wave. In the high-frequency resonance frequency band, where incident wave frequency is consistent with the natural frequency of the soil column above the tunnel, the dynamic stress concentration effect is more significant when it is smaller. The dynamic stress concentration factor inside the lining decreases gradually as the viscosity coefficient increases. The spatial distribution and the displacement amplitudes of surface displacement near the tunnel change as incident wave frequency and angle increase. The effective dynamic analysis of the underground structure under an actual strong dynamic load should consider the slip effect at the lining-surrounding rock interface.vi
dc.language.isoenvi
dc.publisherHindawi Limitedvi
dc.subjectSuperpositionvi
dc.subjectBoundary element methodvi
dc.subjectDynamic responsevi
dc.subjectUnderground structuresvi
dc.subjectStress concentrationvi
dc.subjectStiffnessvi
dc.subjectSlipvi
dc.subjectHoop stressvi
dc.subjectBoundary conditionsvi
dc.subjectFrequenciesvi
dc.subjectTunnel liningsvi
dc.subjectViscosityvi
dc.subjectStress distributionvi
dc.subjectBoundary integral methodvi
dc.subjectComputer simulationvi
dc.subjectPropagationvi
dc.subjectSpatial distributionvi
dc.subjectDynamic loadsvi
dc.subjectStudiesvi
dc.subjectIntegral equationsvi
dc.subjectIncident wavesvi
dc.titleIBIEM Analysis of Dynamic Response of a Shallowly Buried Lined Tunnel Based on Viscous-Slip Interface Modelvi
dc.typeOthervi
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