完整後設資料紀錄
DC 欄位語言
dc.contributor.authorLin, Cheng-Hanen_US
dc.contributor.authorLi, Hung-Huien_US
dc.contributor.authorWeng, Meng-Chiaen_US
dc.date.accessioned2019-04-02T05:58:35Z-
dc.date.available2019-04-02T05:58:35Z-
dc.date.issued2018-09-04en_US
dc.identifier.issn0013-7952en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.enggeo.2018.07.005en_US
dc.identifier.urihttp://hdl.handle.net/11536/148089-
dc.description.abstractA dip slope contains weak planes in the same dip direction along the slope face. In this study, a discrete element simulation was implemented to investigate the behavior of a dip slope under shaking table tests. The simulated dip slope model was first verified by testing under different horizontal excitations. Then, the influence of the slope angle and dynamic force on the deformation characteristics of the dip slopes was explored. The simulations provide detailed descriptions of the deformation processes and potential sliding mechanisms associated with the dip slopes. The results of this study are summarized as follows: (1) Two types of slope sliding, namely differential and complete, were recognized. The model with a dip angle lower than 20 degrees was more stable, and differential sliding developed gradually during external excitation. In the model with a dip angle higher than 20 degrees, the external excitation easily triggered complete sliding. (2) For threshold slope angles higher than 20 degrees, the behavior of the dip slope model changed from deformation to sliding, and the displacement within the models increased with increasing slope angle. (3) An increase in frequency led to a decrease in the trigger time for slope sliding. In addition, the slope angle was negatively correlated with the triggering time for sliding. (4) The amplification factor of peak ground displacement (PGD) increased as the slope angle increased. The amplification factors corresponding to low excitation frequencies were considerably lower than those for high excitation frequencies. In contrast to the trends for PGD, the amplification factor of peak ground acceleration (PGA) decreased as the slope angle increased.en_US
dc.language.isoen_USen_US
dc.subjectDip slopeen_US
dc.subjectDiscrete element methoden_US
dc.subjectSliding modeen_US
dc.subjectShaking table testen_US
dc.titleDiscrete element simulation of the dynamic response of a dip slope under shaking table testsen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/j.enggeo.2018.07.005en_US
dc.identifier.journalENGINEERING GEOLOGYen_US
dc.citation.volume243en_US
dc.citation.spage168en_US
dc.citation.epage180en_US
dc.contributor.department土木工程學系zh_TW
dc.contributor.departmentDepartment of Civil Engineeringen_US
dc.identifier.wosnumberWOS:000443670600016en_US
dc.citation.woscount3en_US
顯示於類別:期刊論文