At mooring DS, the overall vertical- and time-averaged buoyancy frequency is
or
, and the Coriolis frequency is
or
. This equates to a critical frequency
of
averaged over a
square around the mooring.
varies depending on the area used to average the topographic slope (
for a
square,
for a
square). In comparison, at mooring DN,
or
, and the Coriolis frequency is
or
, leading to
.
The difference in
between the 2 moorings (
) is significantly larger than the
confidence interval of
and
for DS and DN, respectively.
Changes in stratification related to mesoscale eddy activity along the Hawaiian Ridge likely would not affect the 3 and 8 month averages at each moorings.
Stratification averages were calculated for each month over the 16 years of CTD data at station ALOHA. No regular annual variations of stratification were observed at the depths of interest (
). We therefore suggest that the difference in
between the 2 moorings is unlikely to be related to the different deployment times (August to November 2002 for DS and November 2002 to June 2003 for DN).
Time-average vertical temperature profiles along
, obtained as part of the World Ocean Circulation Experiment (WOCE), do not show a meridional change large enough on either side of the ridge, although the data are too sparse for a definitive comparison.
The implications of the different stratification at the two moorings will be discussed in section 7 in regards to turbulent dissipation and mixing.
Also, at all depths, absolute temperatures at the moorings are within
of the climatological absolute temperature values (16 years of repeat CTD profiles) at nearby station ALOHA (Figure 2.3).
The Temperature-Salinity (TS) diagrams for the two moorings indicate the similarity of water mass properties on either side of the Ridge (Figure 2.4). The more elongated cloud of TS points at mooring DS compared to DN is related to the higher vertical excursions measured on the south flank. The narrow distribution of T and S allowed us to infer the salinity at depths where only temperature was measured. We used the measured temperature and the inferred salinity to calculate potential density. In chapter 6, we used these potential density profiles to detect statically unstable patches and to estimate turbulent dissipation.
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