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Identifying boundary between near field and far field in ground vibration caused by surface loading 被引量:3

Identifying boundary between near field and far field in ground vibration caused by surface loading
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摘要 The boundary between the near and far fields is generally defined as the distance from the vibration source beyond which ground vibrations are mainly dominated by Rayleigh waves. It is closely related to the type of vibration source and the soil properties. Based on the solutions of the Lamb's problem, the boundary at the surface between the near and far fields of ground vibration was investigated for a harmonic vertical concentrated load and an infinite line load at the surface of a visco-elastic half-space. Particularly, the variation of the boundary with the material damping was investigated for both cases. The results indicate that the material damping slightly contributes to the attenuation of vibrations in the near-source region, but significantly reduces the vibrations in the region that is at some distance away from the source. When taking the material damping into consideration, the boundary between the near and far fields tends to move towards the vibration source. Compared with the vibrations caused by a concentrated load, the vibrations induced by an infinite line load can affect a larger range of the surrounding environment, and they attenuate more slowly. This means the boundary between the near field and far field should move fitrther away from the source. Finally, the boundaries are defined in terms of R-wave length (2R) and Poisson ratio of the ground (o). For the case of a point load, the boundary is located at the distance of (5.0-6.0)2R for v≤0.30 and at the distance of (2.0--3.0)2R for v≥0.35. For the case of an infinite line load, the boundary is located at the distance (5.5-6.5)2rt for v≤0.30 and at the distance (2.5--3.5)2R for v≥0.35. The boundary between the near and far fields is generally defined as the distance from the vibration source beyond which ground vibrations are mainly dominated by Rayleigh waves.It is closely related to the type of vibration source and the soil properties.Based on the solutions of the Lamb's problem,the boundary at the surface between the near and far fields of ground vibration was investigated for a harmonic vertical concentrated load and an infinite line load at the surface of a visco-elastic half-space.Particularly,the variation of the boundary with the material damping was investigated for both cases.The results indicate that the material damping slightly contributes to the attenuation of vibrations in the near-source region,but significantly reduces the vibrations in the region that is at some distance away from the source.When taking the material damping into consideration,the boundary between the near and far fields tends to move towards the vibration source.Compared with the vibrations caused by a concentrated load,the vibrations induced by an infinite line load can affect a larger range of the surrounding environment,and they attenuate more slowly.This means the boundary between the near field and far field should move further away from the source.Finally,the boundaries are defined in terms of R-wave length(λR) and Poisson ratio of the ground(υ).For the case of a point load,the boundary is located at the distance of(5.0-6.0)λR for υ≤0.30 and at the distance of(2.0-3.0)λR for υ≥0.35.For the case of an infinite line load,the boundary is located at the distance(5.5-6.5)λR for υ≤0.30 and at the distance(2.5-3.5)λR for υ≥0.35.
出处 《Journal of Central South University》 SCIE EI CAS 2014年第8期3284-3294,共11页 中南大学学报(英文版)
基金 Project(51178342)supported by the National Natural Science Foundation of China Project(KLE-TJGE-C1301)supported by the Key Laboratory of Geotechnical and Underground Engineering of Ministry of Education(Tongji University)under the International Cooperation and Exchange Program,China
关键词 BOUNDARY near field far field active isolation passive isolation visco-elastic half-space concentrated load line distributed load 阻尼边界 地面振动 表面负荷 远场 近场 Rayleigh波 标识 粘弹性半空间
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