Velocities continued |
Current-meter records were used with the GEM relative-velocity
sections to produce absolute-velocity sections. The GEM method
produces time series of relative (baroclinic, geostrophic) velocity.
But at a given site a single current-meter time series includes the
missing barotropic component of the flow. To minimize error from
ageostrophic components in the current-meter records, the GEM
relative-velocity profile time series were referenced at each mooring
to the deepest current meter without large gaps in its time series.
All current meters used for referencing were below 1000 dbar with one
exception: at the shallowest mooring site, a single current meter was
deployed at 690 dbar. For times when current meters failed, the
relative velocity profiles were referenced to the 1800 dbar time-mean
of these absolute-velocity profiles. This pressure level was used for
referencing because it is deep and has a mean transport per unit depth
near zero. Two gaps, one of 25 days and one of 35 days, persist in
the absolute-velocity section time series, because of the failure of
current meters at mooring sites inshore of IES6; here velocities are
higher and using a mean reference may be less accurate.
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From these absolute-velocity section time series, several time mean
sections were calculated. Shown below are the mean absolute-velocity
fields for (a) times when all referencing current meters were working
and IES8 was deployed, and (b) the entire record.
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Mean velocity section for a 153-day period between November of 1993
and April of 1994. The contour interval is 0.1 m/s. Contours of
eastward flow (thick solid lines), zero flow (solid lines), and
westward flow (dashed lines) are drawn. Light shading indicates the
region of westward flow. Darker shading indicates topography. The
horizontal axis is distance from Cape Ashizuri along the ASUKA line.
This field was made by linear interpolation and extrapolation from the
means of the eight calculated velocity profile time series. This mean
field may have missed a region of westward flow near the base of
the continental slope. The GEM technique fails at depth on the slope
because of the limited number of available deep hydrographic casts on
the slope and because the strong westward flows are not stationary on
a stream coordinate axis.
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Mean velocity section for a 672-day period between November of 1993
and November of 1995. The contour interval is 0.1 m/s. Contours of
eastward flow (thick solid lines), zero flow (solid lines), and
westward flow (dashed lines) are drawn. Light shading indicates the
region of westward flow. Darker shading indicates topography. The
horizontal axis is distance from Cape Ashizuri along the ASUKA line.
This field was made by linear interpolation and extrapolation from the
means of the seven or eight calculated velocity profile time series.
This mean field may have missed a region of westward flow near
the base of the continental slope. The GEM technique fails at depth
on the slope because of the limited number of available deep
hydrographic casts on the slope and because the strong westward flows
are not stationary on a stream coordinate axis.
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The difference between these two mean sections is caused by the
meandering of the Kuroshio. The portion of the ASUKA study when all
referencing current meters were working and IES8 was deployed was a
153-day interval in which the only meander which occurred was a single
little meander of short duration. The 153-day interval shows the mean
velocity section of the Kuroshio in a non-meander state. In contrast,
the entire record mean (672 days) averages together intervals of the
non-meander state, and several intervals of big and little meanders.
This causes the positive velocity contours to spread further offshore
and reduces the mean speeds in the Kuroshio core. The time periods of
meanders of the Kuroshio can be found from the temperature section
time series as will be shown in the transport section of this poster.
Using this information, mean sections for meander periods and for
non-meander periods were calculated.
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Mean velocity section for the 200 days when the Kuroshio was
meandering during the ASUKA study. The contour interval is 0.1 m/s.
Contours of eastward flow (thick solid lines), zero flow (solid
lines), and westward flow (dashed lines) are drawn. Light shading
indicates the region of westward flow. Darker shading indicates
topography. The horizontal axis is distance from Cape Ashizuri along
the ASUKA line. This field was made by linear interpolation and
extrapolation from the means of the seven or eight calculated velocity
profile time series.
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Mean velocity section for 472 days between November of 1993 and
November of 1995 excluding times of Kuroshio meanders. The contour
interval is 0.1 m/s. Contours of eastward flow (thick solid lines),
zero flow (solid lines), and westward flow (dashed lines) are drawn.
Light shading indicates the region of westward flow. Darker shading
indicates topography. The horizontal axis is distance from Cape
Ashizuri along the ASUKA line. This field was made by linear
interpolation and extrapolation from the means of the seven or eight
calculated velocity profile time series. This mean field may have
missed a region of westward flow near the base of the continental
slope. The GEM technique fails at depth on the slope because of the
limited number of available deep hydrographic casts on the slope and
because the strong westward flows are not stationary on a stream
coordinate axis.
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The non-meander mean section is very similar to the 153-day mean. The
missing -0.1 velocity recirculation in the non-meander mean is
probably due to the lower resolution during the time period following
the recovery of IES8. The widening and weakening of the Kuroshio core
in the meander section mean are at least partially due to the turning
of the Kuroshio as it moves on- and off-shore. When the Kuroshio is
not perpendicular to the ASUKA line, the Kuroshio velocities will
appear weaker and the width of the Kuroshio will appear to expand.
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