uplift and subsidence into account, and
assuming global sea-level rise of about 1 m towards the end of the century, the
relative sea-level change will range from a 40–60 cm rise in subsidence regions
to 10–180 cm sea-level drop-in regions of fast uplift. There is considerable
uncertainty in these estimates, with easily justifiable revisions of additional
25–40 cm of sea-level rise. However
/climatology/iceland/climate-report/
with constant stress drop. The radius is given by
wMw
M
MC 5.03
1.9
3 0 10
16
107
16
7
)( σσ Δ
⋅=Δ= , (4)
where ∆σ is the stress drop (see Appendix A and Hanks Kanamori, 1979). In the last term the
seismic moment has been replaced by 101.5M+9.1. When g = 0.5 the form R = r + K·C(M) gives
equivalent results to the form R = r + k·10g·M when fitted to the data – the only difference
between
/media/vedurstofan/utgafa/skyrslur/2009/VI_2009_012.pdf
The lowest layers had a cloud ceiling of 2000 feet, the second layer between 6000-9000 and a third layer at flight level around 19000 feet. The clouds slowly dissipated to the south.
The flight was directed to the northeast from Reykjavik airport, north towards Hofsjokull and Askja. A large circle was then flown around the Bárðarbunga caldera and Holuhraun. In the later part of the flight the area
/earthquakes-and-volcanism/articles/nr/3011
Over the western part of Iceland the cloud cover was broken and layered. The lowest layers
had a cloud ceiling of 2000 feet, the second layer between 6000-9000 and a third layer at
flight level around 19000 feet. The clouds slowly dissipated to the south.
The flight was directed to the northeast from Reykjavik airport, north towards Hofsjokull and
Askja. A large circle was then flown around
/media/jar/Bardarbunga-2014_October-events.pdf
The lowest layers had a cloud ceiling of 2000 feet, the second layer between 6000-9000 and a third layer at flight level around 19000 feet. The clouds slowly dissipated to the south.
The flight was directed to the northeast from Reykjavik airport, north towards Hofsjokull and Askja. A large circle was then flown around the Bárðarbunga caldera and Holuhraun. In the later part of the flight the area
/earthquakes-and-volcanism/articles/nr/3011/
m
J
M5 [C°] -3
obs. [C°] -4
nce 1
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/media/ces/2010_017.pdf
The hydrological simulations were performed with the Wa-
tershed Simulation and Forecasting System (WSFS) developed
and operated in the Finnish Environment Institute (Vehviläinen
et al., 2005). The WSFS is used in Finland for operational hydrolog-
ical forecasting and flood warnings (www.environment.fi/water-
forecast/), regulation planning and research purposes
(Vehviläinen and Huttunen, 1997
/media/ces/Journal_of_Hydrology_Veijalainen_etal.pdf
Percolating water from the melt-
ing snow may have increased the rate of movement. Seismic data
indicate that a sudden movement occurred around 40 minutes be-
fore the slide, but at 23:24 the failure point was reached and the
rockslide was released.
? Width of fracture line: 800 m
? Vertical drop: 350 m
? Run-out length beyond the lake shore: ~1000 m
? Volume: ~30–50 million m³
? Estimated
/media/vedurstofan/utgafa/skyrslur/2015/IMO_AnnualReport2014.pdf
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/media/loftslag/Hare-2011-ParticipatoryModelling.pdf