Quick
Search: 
 
advanced search
 GSW Home    GeoRef Home    My GSW Alerts    Contact GSW    About GSW    Journals List    Help 
  Quarterly Journal of Engineering Geology & Hydrogeology   Don't get GSW? Talk to your librarian.
JOURNAL HOME HELP CONTACT PUBLISHER SUBSCRIBE ARCHIVE SEARCH TABLE OF CONTENTS

Quarterly Journal of Engineering Geology & Hydrogeology; May 2006; v. 39; no. 2; p. 115-129; DOI: 10.1144/1470-9236/05-041
© 2006 Geological Society of London
This Article
Right arrow Figures Only
Right arrow Full Text
Right arrow Full Text (PDF)
Right arrow Alert me when this article is cited
Right arrow Alert me if a correction is posted
Services
Right arrow Email this article to a friend
Right arrow Similar articles in this journal
Right arrow Alert me to new issues of the journal
Right arrow Download to citation manager
Citing Articles
Right arrow Citing Articles via HighWire
Right arrow Citing Articles via Web of Science (8)
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by Davies, T.R.
Right arrow Articles by Beetham, R.D.
Right arrow Search for Related Content
GeoRef
Right arrow GeoRef Citation

Rapid block glides: slide-surface fragmentation in New Zealand's Waikaremoana landslide

T.R. Davies1, M.J. McSaveney2 and R.D. Beetham2

1 1Department of Geological Sciences, University of Canterbury, Christchurch, New Zealand(e-mail: tim.davies@canterbury.ac.nz)
2 2GNS Science, Lower Hutt, New Zealand

Physical modelling of part of prehistoric Waikaremoana landslide shows that the blockslide must have hit the valley wall at c. 40 m/s, after sliding 2 km on a 5.5–8° slope, in order to form the 150-m high mound of debris known as Raekahu. Both the blockslide and a distal rock avalanche were in simultaneous motion when the impact occurred. Finely ground rock on the slide plane suggests that a mechanism of dynamic rock fragmentation may explain the low friction necessary for acceleration to 40 m/s. When a rock particle fractures in a confined space, an isotropic dispersive pressure equal to the rock's Hugoniot elastic limit (in the GPa range) at the ambient pressure and strain rate may be exerted on its surroundings. Beneath the 275-m thick block, about one particle in 15–30 or so fragmenting at any instant (with lower density for higher rock strength at higher strain rate), could completely support the weight of the block by fragmentation pressure; but then there would be no frictional resistance (and hence no further fragmentation). Self-regulation of the process may explain the apparent coefficient of friction of c. 0.1 in the blockslide. Low friction through dynamic fragmentation may apply widely to blockslides with a basal layer of comminuted rock.

Key Words: Block glide • dynamic fragmentation • physical model • Waikaremoana landslide • New Zealand • landslide mechanism • low friction




This article has been cited by other articles:


Home page
Geological Society, London, Special PublicationsHome page
C. Boulton, T. Davies, and M. McSaveney
The frictional strength of granular fault gouge: application of theory to the mechanics of low-angle normal faults
Geological Society, London, Special Publications, January 1, 2009; 321(1): 9 - 31.
[Abstract] [Full Text] [PDF]




JOURNAL HOME HELP CONTACT PUBLISHER SUBSCRIBE ARCHIVE SEARCH TABLE OF CONTENTS
Copyright © 2009 by Geological Society of London