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Surprisingly, the ADCP, normally oriented downward,
was inverted (upward -looking) during the ~1/2 h peak flow during
event 2. Tilt and pitch
of the ADCP also indicate significant deflection of the mooring during
these events. Modeling of the drag on the mooring components indicated
that maximum speeds of ~3.6 m/s were required to defect the mooring
toward the seafloor by 25 m (Figure 5).
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Figure 5
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There is some evidence that the mooring
was moved during these events. The
long term depth record from the ADCP (Figure
1, second panel) shows
that the mooring depth increased after the second event, apparently
due both to the added weight of the entrained sediment in the sediment
trap, as well as movement of up to 200 m of the entire mooring (based
on deployment and recovery navigation). The mooring slowly rose in depth a week or so after event 2,
suggesting that some of the sediment load fouling the mooring was
flushed during high tidal currents during spring tides. However, the rapid increase in the depth of the mooring
observed during mid-March 2003 is not associated with other anomalous
data and is presently inexplicable.
Although rapid current speeds
persisted for at most a few hours, suspended sediment was above normal
for a day or more. Optical
backscatter (detected by a HOBI Labs HS2) showed that suspended
sediment was above normal for >24 h (Figure
2). Backscatter strength reported by the ADCP (not shown) also
showed that these events were detectable for several days. Fluorescence also increased during these events, but not to the
degree detected during other periods, suggesting that the chlorophyll
signal was simply part of the suspended material entrained in the
turbidity flow.
Temperature increased immediately
during these events, with peak temperatures of 5.3 and 3.8 degrees C
at the beginning of events 1 and 2, respectively. High temperatures are caused by the shallower, warmer water
entrained in the turbidity flow and transported down-canyon. Using these temperature data, we can calculate a conservative
estimate of the origin of the flow can be made from its temperature. Event 1, with a temperature of 5.3 oC, must have
originated in ~630 m depth or shallower (based on a typical
temperature profile from central Monterey Bay), since mixing and heat
loss occurs during the turbidity flow. Event 2 may have originated nearer our mooring (~900 m), since
its temperature anomaly is lower. Alternatively, the smaller T-anomaly of event 2 may indicate a
more distant source, which underwent greater mixing and dilution
before reaching our mooring. Moreover,
it is possible that each event originated near our mooring on the
walls of the canyon, and entrained shallower, warmer water as the
turbid flow sank to the axis and flowed down-canyon. A location in the axis of Monterey Canyon at 630 m depth is ~20
km “up-canyon” from the benthic mooring, suggesting that these
events traveled a considerable distance.
Loss of RINs and BINs from the
Canyon Dynamics site (yellow squares on map) during these events
indicated that the same event(s) that impacted the Canyon Dynamics
site continued through the canyon to our mooring, a distance of at
least 25-30 km.
Was the event confined to the
canyon? Apparently so. Although we have no other current speed data from outside the
canyon, another sediment trap was deployed on Smooth Ridge in 1300 m
depth (~20 km from the canyon mooring). This sediment trap showed low sediment flux and no anomalous
sedimentation events during the same period.
What initiated this turbidity
flow? For the 2001 event
(Paull et al), no clear signal was related to the turbidity flow.
For this event, however, a huge storm with 6 m waves lasted for
several days prior to, and during, these events (Figure
1,2).
This is the same storm that detached the MOOS mooring only days
earlier.
How frequent are turbidity
events in Monterey Canyon? In
addition to the Christmas events that occurred during the past 2
years, the RINs & BINs of the Canyon Dynamics Project were moved
by turbidity flows during summer 2002, and apparently again in March,
2003. This is considerably more
frequent that expected, with large volumes of sediment transported in
these events. The MOOS Science Experiments, planned for
2004/2005 will attempt to measure the flow of materials and carbon in
the lower canyon near Shepard Meander near 3500 m. It will be
interesting to see if the upper canyon events penetrate to near the
abyssal plain.
Oceanographic El Nino events were named originally for warm water that
would arrive around Christmastime off the coast of Peru. We’ll
be ready for this year’s "El Nino Event" in the canyon,
but our mooring will have an even larger anchor weight.
June 2003

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