dc.contributor.author |
Voyagaki, E |
en |
dc.contributor.author |
Mylonakis, G |
en |
dc.contributor.author |
Psycharis, IN |
en |
dc.date.accessioned |
2014-03-01T02:51:48Z |
|
dc.date.available |
2014-03-01T02:51:48Z |
|
dc.date.issued |
2008 |
en |
dc.identifier.issn |
08950563 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/35664 |
|
dc.subject.other |
Analytical and numerical solutions |
en |
dc.subject.other |
Closed form solutions |
en |
dc.subject.other |
Closed-form expression |
en |
dc.subject.other |
Frictional strength |
en |
dc.subject.other |
Geotechnical engineers |
en |
dc.subject.other |
Ground accelerations |
en |
dc.subject.other |
Ground motions |
en |
dc.subject.other |
Ground velocity |
en |
dc.subject.other |
Near-fault |
en |
dc.subject.other |
Near-fault earthquake |
en |
dc.subject.other |
Peak displacement |
en |
dc.subject.other |
Peak response |
en |
dc.subject.other |
Permanent displacements |
en |
dc.subject.other |
Plastic response |
en |
dc.subject.other |
Pulse waveforms |
en |
dc.subject.other |
Residual soil |
en |
dc.subject.other |
Rigid block |
en |
dc.subject.other |
Rupture directivity |
en |
dc.subject.other |
Salient features |
en |
dc.subject.other |
Sliding blocks |
en |
dc.subject.other |
Time history |
en |
dc.subject.other |
Wave forms |
en |
dc.subject.other |
Civil engineering |
en |
dc.subject.other |
Earthquakes |
en |
dc.subject.other |
Engineering |
en |
dc.subject.other |
Engineering geology |
en |
dc.subject.other |
Friction |
en |
dc.subject.other |
Soil structure interactions |
en |
dc.subject.other |
Soils |
en |
dc.subject.other |
Geotechnical engineering |
en |
dc.title |
Sliding blocks under Near-fault pulses: Closed-form solutions |
en |
heal.type |
conferenceItem |
en |
heal.identifier.primary |
10.1061/40975(318)130 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1061/40975(318)130 |
en |
heal.publicationDate |
2008 |
en |
heal.abstract |
Analytical and numerical solutions are presented for the rigid-plastic response of geo-structures to idealized ground acceleration pulses. These shock-like waveforms are typical of near-fault earthquake motions generated by forward fault-rupture directivity and may inflict large permanent displacements in the absence of substantial residual soil strength. The geo-structures are modeled as rigid blocks resting on inclined frictional planes. Although idealized, these models are widely accepted by geotechnical engineers, for simulating a variety of structures including retaining walls, embankments and slopes. Four basic simple pulse waveforms are examined: (1) rectangular; (2) sinusoidal; (3) triangular; (4) exponential. An analytical study is presented on the effect of frictional strength and number of excitation cycles on peak displacements. Results are presented in the form of dimensionless graphs and closed-form expressions that elucidate the salient features of the problem. It is shown that Newmark approaches based on conventional motions may under- or over-estimate peak displacements depending on the circumstances. It is also shown that all three time histories of ground motion (i.e., acceleration, velocity, and displacement) control peak response - contrary to the widespread view that ground velocity alone is of leading importance. Issues related to scaling laws of peak displacement are discussed. © 2008 ASCE. |
en |
heal.journalName |
Geotechnical Special Publication |
en |
dc.identifier.doi |
10.1061/40975(318)130 |
en |
dc.identifier.issue |
181 |
en |