Radiating away from the summits of Hawaiian volcanoes are
(usually two) linear rift zones. The rift zones conspicuously
do not point towards adjacent volcanoes, but instead parallel
the volcano-volcano boundaries. Rift zones mark
preferred directions
of sub-horizontal magma excursions from the magma chamber.
At
the surface they are characterized by numerous vents, fissures,
earth cracks, cinder cones, graben, pit craters, and the sources
of lava flows. All of these are indications that magma preferentially
intrudes into the rift zones and is also often stored there for
periods of time up to a few years.
There has been much discussion about the formation and persistence
of Hawaiian rift zones (e.g.
Fiske & Jackson 1972;
Deterich 1988).
The general idea is that because Hawaiian volcanoes are close
to one another relative to their size, a younger volcano is
growing
through the flank of an older one. The gravitational stress field
caused by the pre-existing volcano tends to yield downslope-directed
directions of least compressive stresses. Because dikes orient
themselves so that their direction of widening is parallel to
this least compressive stress, the dikes end up propagating parallel
to the volcano-volcano boundary. Once a preferred direction of
dike propagation is established, it is self-perpetuating as long
as there is a mechanism for the flanks of a volcano to move outward
to accommodate the repeated dike injections. The most popular
mechanism for this outward movement is
sliding along the volcano-ocean
floor interface which consists of easily-deformable sediments
(e.g. Nakamura 1982).
The focal mechanism for the 1975 M7.2 Kalapana earthquake indicated
a slip plane that was nearly horizontal with a slight dip towards
at a depth consistent with the base of the volcano (e.g.
Lipman et al. 1985).
Such an orientation would be expected due to the downward warping
of the oceanic lithosphere under the load of the island.
Rift zones probably become preferred directions of dike propagation
due to stress orientations, and they evolve thermally to perpetuate
themselves. This means that eruptions are rare elsewhere on the
flanks of the shields. Except at the summit, the vents of Kilauea
are found exclusively along the rift zones. On Mauna Loa, however,
there is a class of vents called "radial vents
" (Lockwood &
Lipman 1987)
that are found on the northern and western flanks. This is the
sector on the obtuse side of the angle formed by the two rift
zones, and circumferential tension caused by a bending moment
set up by the rift zones and the westward push of neighboring
may be leading to the formation of these vents
(Walker 1990).
Probably the most studied rift zone is the east rift of Kilauea.
The northern flank of this rift is stable, probably because it
abuts Mauna Loa. The south flank, however, is notably mobile.
It has been shown to move seaward during both earthquakes and
intrusive events. There is nothing in this direction to buttress
the flank so the continued pressure caused by numerous dike intrusions
produces this seaward displacement
(Swanson et al. 1976;
Lipman et al. 1985).
This relative displacement between the non-mobile north flank
and mobile south flank has caused a wide graben to form along
the crest of the rift. Thus even though the rift axis is the locus
of most eruptive activity it is in places topographically subdued.
Some of the faults bounding this graben are visible near
Napau
crater.
Pit Craters:
Continued transport of magma down the rift zone results in
the establishment of a thermally efficient conduit probably 2-3
km below the surface. Some evidence for this was provided by the
first 10 km of propagation of the dike marking the onset of the
Pu'u 'O'o/Kupa'ianaha eruption being aseismic
(Klein et al. 1987).
This indicates that there was a pre-existing conduit could be
utilized by the migrating magma. This distance corresponds rather
closely with the distribution of pit craters along the east rift
Kilauea. Beyond the first 10 km, earthquakes marked the propagation
of the dike.
Pit craters are not explosion craters or vents, but rather
they are locations of localized collapse into a void.
The above-mentioned
conduit is the best candidate for such a void. A pit crater forms
from the bottom up by stoping of a cavity. Evidence for this is
provided by a pit crater called the
"Devil's Throat."
When first noticed by Westerners, Devils Throat was a hole in
the ground a few 10's of m across. A very brave man was lowered
through this opening on a winch, and he soon found himself in
a huge cavity, much wider than the hole he'd come through. It
was evident that he was in a bell-shaped void and that the top
layers of lava had not yet collapsed into it. Since then the last
layers have fallen in, leaving Devil's Throat with the more typical
cylindrical form of a pit crater. Eruptive fissures occasionally
cut right across pit craters apparently without noticing the difference
in topography. An eruptive fissure can extend from the
floor of
a pit crater, up the wall, and continue on beyond the rim.
In summary, vent, graben, and pit crater distributions yield
insight to the preferred directions of magma travel within a Hawaiian
volcano. These in turn can yield information about the stress
directions within the edifice
(e.g. McGuire & Pullen
1989;
Rubin 1990).
There have been some attempts to tie these stress directions to
the stress field within the Pacific plate but it appears that
the local stress field caused by neighboring volcanoes is much
more important in determining the eventual direction of rift zone
formation.
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