scholarly journals Modeling the dynamic response of a crater glacier to lava-dome emplacement: Mount St Helens, Washington, USA

2007 ◽  
Vol 45 ◽  
pp. 21-28 ◽  
Author(s):  
Stephen F. Price ◽  
Joseph S. Walder

AbstractThe debris-rich glacier that grew in the crater of Mount St Helens after the volcano’s cataclysmic 1980 eruption was split in two by a new lava dome in 2004. For nearly six months, the eastern part of the glacier was squeezed against the crater wall as the lava dome expanded. Glacier thickness nearly doubled locally and surface speed increased substantially. As squeezing slowed and then stopped, surface speed fell and ice was redistributed downglacier. This sequence of events, which amounts to a field-scale experiment on the deformation of debris-rich ice at high strain rates, was interpreted using a two-dimensional flowband model. The best match between modeled and observed glacier surface motion, both vertical and horizontal, requires ice that is about 5 times stiffer and 1.2 times denser than normal, temperate ice. Results also indicate that lateral squeezing, and by inference lava-dome growth adjacent to the glacier, likely slowed over a period of about 30 days rather than stopping abruptly. This finding is supported by geodetic data documenting dome growth.

2007 ◽  
Vol 45 ◽  
pp. 14-20 ◽  
Author(s):  
Joseph S. Walder ◽  
Richard G. LaHusen ◽  
James W. Vallance ◽  
Steve P. Schilling

AbstractThe process of lava-dome emplacement through a glacier was observed for the first time after Mount St Helens reawakened in September 2004. The glacier that had grown in the crater since the cataclysmic 1980 eruption was split in two by the new lava dome. The two parts of the glacier were successively squeezed against the crater wall. Photography, photogrammetry and geodetic measurements document glacier deformation of an extreme variety, with strain rates of extraordinary magnitude as compared to normal alpine glaciers. Unlike normal temperate glaciers, the crater glacier shows no evidence of either speed-up at the beginning of the ablation season or diurnal speed fluctuations during the ablation season. Thus there is evidently no slip of the glacier over its bed. The most reasonable explanation for this anomaly is that meltwater penetrating the glacier is captured by a thick layer of coarse rubble at the bed and then enters the volcano’s groundwater system rather than flowing through a drainage network along the bed.


2008 ◽  
pp. 225-236 ◽  
Author(s):  
Michael P. Poland ◽  
Daniel Dzurisin ◽  
Richard G. LaHusen ◽  
Jon J. Major ◽  
Dennis Lapcewich ◽  
...  

2008 ◽  
pp. 257-276 ◽  
Author(s):  
Joseph S. Walder ◽  
Steve P. Schilling ◽  
James W. Vallance ◽  
Richard G. LaHusen

2008 ◽  
pp. 145-167 ◽  
Author(s):  
Steve P. Schilling ◽  
Ren A. Thompson ◽  
James A. Messerich ◽  
Eugene Y. Iwatsubo

Author(s):  
A. Christou ◽  
J. V. Foltz ◽  
N. Brown

In general, all BCC transition metals have been observed to twin under appropriate conditions. At the present time various experimental reports of solid solution effects on BCC metals have been made. Indications are that solid solution effects are important in the formation of twins. The formation of twins in metals and alloys may be explained in terms of dislocation mechanisms. It has been suggested that twins are nucleated by the achievement of local stress-concentration of the order of 15 to 45 times the applied stress. Prietner and Leslie have found that twins in BCC metals are nucleated at intersections of (110) and (112) or (112) and (112) type of planes.In this paper, observations are reported of a transmission microscope study of the iron manganese series under conditions in which twins both were and were not formed. High strain rates produced by shock loading provided the appropriate deformation conditions. The workhardening mechanisms of one alloy (Fe - 7.37 wt% Mn) were studied in detail.


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