Earth and Planetary Science Letters, 102 (1991) 413-429 413
Elsevier Science Publishers B.V., Amsterdam
[XLeP]
Gas content, eruption rate and instabilities of eruption regime
in silicic volcanoes
Claude Jaupart and Claude J. All6gre
Unioersitd Paris 7 et Institut de Physique du Globe de Paris, 4 place Jussieu, 75252 Paris Cedex 05, France
Received April 23, 1990; revised version accepted September 3, 1990
ABSTRACT
In silicic volcanoes, eruptions commonly begin with violent explosive phases and evolve towards a regime of dome
formation. This transition is characterized by a decrease of gas volume fraction, which has usually been attributed to chemical
gradients in the volcano chamber. Petrological and geochemical studies suggest that this interpretation may be oversimplified.
A critical observation is that the eruption rate decreases with time and is markedly smaller during dome growth than during
explosive activity. Following Eichelberger et al. [1], we suggest that the transition from explosive activity to dome formation is
due to gas loss through permeable conduit walls. Further, in some cases, the same process may be responsible for the
transition from the ash fall regime to pyroclastic flows. Both transitions are a direct consequence of a decrease of eruption rate
at constant conduit radius. The gas content of lava rising towards the Earth's surface is determined by two competing
processes: pressure release leading to gas exsolution and expansion, and gas loss to the country rock. The amount of gas lost is
inversely proportional to the eruption rate and proportional to the pressure difference between conduit and country rock. The
critical variable is the pressure in the volcano chamber. This pressure steadily decreases with time as the chamber empties,
implying a decrease of eruption rate. In turn, this decrease acts to increase the fraction of gas lost to the country rock and
hence to reduce the gas content of the erupted material. The model therefore predicts that, with time, the eruption undergoes a
transition from explosive to non-explosive conditions. These transitions occur as bifurcations in the evolution of gas volume
fraction with height in the conduit. We find that very small pressure fluctuations of the order of one bar in the chamber lead
to large changes of gas content at the vent. This suggests that the transitions of eruptive regime are unstable, and provides an
explanation for observed alternations between explosive phases and dome formation. With time, such pressure fluctuations
occur when the average vesicularity is smaller and may manifest themselves by extrusion events through an existing dome.
In Appendix B, we use data on the height of the Montagne Pelre spine in 1902 and 1903 to show that the pressure driving
this eruption decreased by about 2 MPa in a year.
1. Introduction
In silicic volcanoes, eruptions commonly begin
with violent explosive phases and end in a regime
of dome formation where degassed lava slowly
spreads out of the vent. These transitions of erup-
tion regime have been observed in many cases [2]
and thus seem to be a fundamental feature of
these volcanoes. The classical explanation of this
behaviour is that the volcano chamber is zoned
with a volatile rich upper part, however this has
been challenged recently in a series of stimulating
papers [1,3]. In the Inyo domes volcanic system,
Eichelberger et al. [1] and Swanson et al. [4] pro-
vided evidence that lava once contained large
amounts of dissolved volatiles and has mineral
assemblages almost identical to those in tephra
from the associated Plinian phase, indicating that
both eruptive phases sampled similar melts. Inde-
pendent support for this suggestion comes from a
study of the nearby Mono craters, which indicate
that, during ascent through the volcanic conduit,
lava and exsolved gas behaved as a closed system
during the Plinian phase and as an open one
during dome extrusion [5]. Thus, the behaviour of
volatiles depends on the eruption regime.
Eichelberger et al. [1] proposed that magma
retains its gas during the initial explosive phase
when the volcanic edifice is intact and then loses it
in the heavily fractured and permeable vent funnel
which develops. Their model focusses on how gas
can flow through a permeable foam and does not
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