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- Lava dome eruptions - overview
- When does dome lava break?
- Shear fracture in conduits and domes
- Fracture, seismicity and degassing
- Mechanisms and consequences of collapse:
- -gravitational collapse
- -collapse due to gas pressurisation
- -rainfall-triggered collapse
- Some unresolved issues…
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- Domes of silica-rich lava (andesite-rhyolite), typically tens-hundreds
of metres high
- Domes grow over months-years, punctuated by collapse events and
explosive eruptions
- Highly hazardous – can generate pyroclastic flows that destroy
settlements on volcano flanks
- High viscosity magma: 106 to 1014 Pa s (due to
high SiO2, plus degassing, crystallisation and cooling)
- Examples include Unzen, Montserrat, Colima, Popo, Merapi & MSH
- Key problem: how to predict dome collapse
- and explosions (e.g. Sparks 2003 EPSL Frontiers)
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- Two styles of dome growth: endogenous and exogenous
- There may be several or dozens of phases of dome growth and collapse:
some endogenous, some exogenous.
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- e.g. Montserrat 1997* e.g. MSH 2004-
- dome inflates from within isolated spines emplaced along shear
zones
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- Will shear zones develop in the dome? If so, an exogenous eruption will
take place.
- But – how do these shear zones form?
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- Deforming magma may either flow or fracture:
- High temperatures, low strain rates: flow
- Lower temperatures, high strain rates: fracture
- This is due to the viscoelasticity of the melt, as described in papers
by Don Dingwell. The transition from liquid-like to solid-like behaviour
in silicate melts is known as
the glass transition
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- The glass transition: flow or fracture in magma
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- From deformation experiments by Dingwell and Webb: silicate melts will
fracture if strain rate ´
viscosity is greater than a certain value (108 Pa).
- This is because viscous flow of the melt is too slow to allow the
stresses to relax – so the stresses rise until the melt fractures.
- We can now think about whether and where magma will fracture!
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- high strain rates and lower temperatures at conduit wall ŕ fracture
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- When will exogenous dome growth occur? – when shear zones propagate from
the conduit wall into the dome (Hale 2005 PhD thesis and 2004 IAVCEI
abstract)
- Shear fracture of magma in the conduit generates these shear zones.
- There is much discussion around how factors such as magma discharge rate
influence this exo/endo- transition…
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- Due to gravitational instability….
- which may or may not be assisted by
- 1) Gas pressurisation of the dome
- or
- 2) Rainfall on the dome surface
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- from Voight (2000) Phil Trans Roy Soc A 358, 1663-1703
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- from Voight (2000) Phil Trans Roy Soc A 358, 1663-1703
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- how much of the dome will collapse?
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- Dome and shallow conduit pressurised by volcanic gases (volatile-rich
magma)
- Tilt cycles – cyclic pressurisation of dome (e.g. Voight et al. 1999
Science)
- At Montserrat, collapse events related to pressurisation…
- But, how did pressurisation lead to collapse?
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- Elsworth and Voight models
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- We have seen that magma fracture has a huge influence on how domes
behave and collapse:
- 1) The formation of shear fractures controls the exogenous-endogenous
transition
- 2)Gravitational failure requires the dome lava to fracture
- 3) If domes do collapse, unloading may trigger explosive fragmentation
of magma in the conduit
- 4) Fracturing also allows gas to escape and triggers shallow volcanic
earthquakes
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- Plenty of unresolved issues that are currently being addressed (work in
progress)….such as
- when is dome growth exogenous/endogenous?
- what is the strength of hot dome lava?
- how is lava strength affected by alteration and cracking?
- how does seismicity link in with dome collapse?
- do earthquakes trigger collapses or vice versa?
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