barotropic’transport’of’the’antarcdc’circumpolar’current ......c01 m01 c02 m02 c03 c04...

1
2.Mean barotropic transport calculated from nearbo6om currents 5. Discussion Karen L. Tracey, Kathleen A. Donohue, and D. Randolph Wa8s 950 1. cDrake experiment [email protected] www.cDrake.org 3. Barotropic transport variability calculated from bo6om pressures References Chidichimo et al. 2014. Baroclinic transport time series of the Antarctic Circumpolar Current in Drake Passage. J. Phys. Oceanogr. (submitted). Cunningham et al. 2003. Transport of the Antarctic Circumpolar Current in Drake Passage. J. Geophys. Res. 108: 8084. Firing et al. 2011. Vertical structure and transport of the Antarctic Circumpolar Current in Drake Passage from direct velocity measurements. J. Geophys. Res. 116: C08015. Koshlyakov et al. 2012. Currents in Drake Passage based on observations in November of 2010. Oceanology. 52: 299-308. Mazloff et al. 2010. An eddy-permitting Southern Ocean State Estimate. J. Phys. Oceanogr. 40: 880-899. Whitworth. 1983. Monitoring the transport of the Antarctic Circumpolar Current at Drake Passage. J. Phys. Oceanogr. 13: 2045-2057. Whitworth and Peterson. 1985.Volume transport of the Antarctic Circumpolar Current from bottom pressure measurements. J. Phys. Oceanogr. 15: 810-816. C17 C16 C15 C14 C13 C12 C11 C10 C09 C08 C07 C06 C19 C05 C20 C04 C03 C02 C01 C17 C16 C15 C14 C13 C12 C11 C10 C09 C08 C07 C06 C19 C05 C20 C04 C03 C02 C01 Correlation 0 0.5 1 Barotropic Transport of the AntarcDc Circumpolar Current Measured in Drake Passage Region Mean (Sv) NS 7.5 (a) NDP 7.7 (a) SFZ 15.9 (b) SDP 15.1 (a) SS 2.3 (c) Total 43.8 Visit other cDrake posters: 951 Foppert et al. Mean baroclinic structure of Polar Front in stream coordinates near Shackleton Fracture Zone. 849 Millar et al. Four-year observations of interfacial form stress in the northern Drake Passage. Energetic transport fluctuations with periods of 50-180 days in SFZ and NDP regions are associated with the main ACC fronts shifting between regions. These fluctuations are nearly equal and opposite, and the variability of total barotropic transport in that period band is reduced. Transport fluctuations with periods in the 50-180 day band are weak at the southern and northern subregions of the passage. C11-C17 pressures, south of the Shackleton Fracture Zone, exhibit less variance than those north of the topographic ridge. Southern pressure records (C17-C11) are highly correlated with one another. 4-year observational period from Nov 2007 to Nov 2011. 42 Current and Pressure recording Inverted Echo Sounders (CPIES) in transport line (solid triangles) and local dynamics array (open triangles). C01-C08 spacing: ~30 km C08-C17 spacing: ~60 km 5 closely-spaced CPIES (H01- H05) along Shackleton Fracture Zone in year 4. 3 short current meter moorings (M01-M03) deployed at continental margins for first 2 years. Bo8om pressures C01 C02 C03 C04 C20 C05 C19 C06 C07 2008 2009 2010 2011 0.2 0 0.2 C08 C09 C10 C11 C12 C13 C14 C15 C16 2008 2009 2010 2011 C17 Leveled and dedrifted using near-bottom currents. Unresolved residual drift (< 1 cm per 1000 days) corresponds to 4 Sv barotropic transport error over a 4-year experiment. Linenormal currents dbar Measured 50 m above the seafloor. Rotated to be perpendicular to the transport line. 3 dlp currents are poorly correlated from site to site, while neighboring 90 dlp currents are positively or negatively correlated. All measurements: 1 hour sampling interval. Tides removed: Semi-diurnal and diurnal using response analysis, fortnightly and lunar monthly tides with TPXO7.2. 3 day low-pass filter applied to hourly samples and subsampled to twice daily. 64 o W 62 o W 60 o W 62 o S 60 o S 58 o S 56 o S 10 cm s 1 64 o W 62 o W 60 o W 62 o S 60 o S 58 o S 56 o S 64 o W 62 o W 60 o W 62 o S 60 o S 58 o S 56 o S SS SDP SFZ NDP NS 0.1 m s 1 64 o W 62 o W 60 o W 62 o S 60 o S 58 o S 56 o S Annual means are remarkably stable from year to year across the whole Drake Passage. This permits variable- record-length means to be used to estimate the barotropic transport and its error. The across-passage mean currents are well resolved by the closely-spaced cDrake array. Standard error ellipses are small compared to the record-length mean currents. Gray contours: 4-year mean SSH from Aviso (c.i. 10 cm). (a) Standard trapezoidal integration. (b) Distance-weighted trapezoidal integration with l = 15 km for H01 and H03. Error estimation allowed l (distance from the Shackleton Fracture Zone) to vary between 10, 15, and 20 km based on LADCP casts taken on cDrake cruises and by Koshlyakov et al. (2012). (c) Distance-weighted trapezoidal integration with l = 24 km for C16. Error estimation was based on l = 24 km (distance from the South Shetland Trench) and l = 36 km (no distance weighting). 4. Total transport through Drake Passage 6. Summary 0.2 0.1 0 0.1 0.2 Line normal velocity (m s 1 ) C17 M03 C16 C15 C14 C13 C11 C10 C09 C08 C07 C06 C19 C05 C20 C04 C03 M02 C02 M01 C01 yr 1 yr 2 yr 3 yr 4 4 yrs 62°S 60°S 58°S 56°S 0 2000 4000 Depth (m) Error EsDmaDon Transport (Sv) Arraywide resoluJon for 90 day lowpassed currents 7.7 CorrelaJon scales near topography in subregion SFZ (b) 2.8 CorrelaJon scales near topography in subregion SS (c) 1.8 Possible bo8om trapping bias (under invesJgaJon) 4 ± 4 Total 9.3 Barotropic transport is calculated using trapezoidal integration of the near-bottom velocity times the site-dependent water depth. The average site depth in the deep passage is about 4000 meters. Five subregions were defined based on topographic features: Northern and Southern Slopes (NS and SS), Shackleton Fracture Zone (SFZ), and Northern and Southern Deep Passages (NDP and SDP). H01-H03 sites were shifted along topography to the transport line to resolve the deep flow near the Shackleton Fracture Zone. The mean eastward transport accumulates beneath the SAF and PF. The mean eastward barotropic transport is 43.8 Sv with an uncertainty of 9.3 Sv. This mean transport translates to a mean across- passage eastward bottom-reference velocity of 1.3 cm s -1 . The cDrake moored array provided measurements across the Drake Passage with high spatial and temporal resolution for four years. Annual mean currents are remarkably stable from year to year and provide robust estimates of the barotropic transport. The mean barotropic transport is 43.8 Sv ± 9.3 Sv. Variability of the barotropic transport is dominated by the variability northward and downstream of the Shackleton Fracture Zone. Summing the barotropic transport with the bottom-referenced baroclinic transport of 127.7 Sv gives a total mean eastward transport of 171.4 Sv through Drake Passage. The variability of the barotopic component accounts for the largest fraction (80%) of the total transport variability. cDrake observations have been assimilated into the Southern Ocean State Estimate (Mazloff et al. 2010). This effort will provide perspective on how the cDrake measurements and derived quantities fit into the context of local, regional and large-scale variability, and their associated forcing. C01 M01 C02 M02 C03 C04 C20 2008 2009 2010 2011 0.4 0 0.4 m s 1 C05 C19 C06 C07 C08 C09 C10 C11 2008 2009 2010 2011 C12 C13 C14 C15 C16 M03 2008 2009 2010 2011 C17 Record-length mean near-bottom currents perpendicular to the transport line were used to determine the mean barotropic transport. J A J O J A J O J A J O J A J O SS SDP SFZ NDP NS Total Barotropic 50 Sv 2008 2009 2010 2011 3 dlp and 90 dlp Transports By Region Transports (Sv) 4 year Mean SEM Std dev Yr 1 Mean Yr 2 Mean Yr 3 Mean Yr 4 Mean Baroclinic + Barotropic 171.4 3.1 18.7 170.1 175.8 177.2 162.7 Baroclinic 127.7 1.0 8.1 128.0 128.5 126.8 127.4 Barotropic 43.8 3.0 18.3 42.2 47.3 50.4 35.3 J A J O J A J O J A J O J A J O 50 0 50 100 150 200 250 Baroclinic + Barotropic Baroclinic Barotropic Transport (Sv) 2008 2009 2010 2011 Full-depth baroclinic transport referenced to zero at the bottom was calculated from the cDrake CPIES records by Chidichimo et al. (2014). While the barotropic component accounts for only 25% of the total transport, with a temporal standard deviation of 18.3 Sv, it accounts for 80% of the total variability observed over the four years. NSF Office of Polar Programs supported this work under grants ANT-0635437 and ANT-1141802. Steady annual mean transports confirm that the 4-year means are robust. Baroclinic component of 127.7 Sv accounts for 75% of the total eastward transport of 171.4 Sv through Drake Passage. Transport fluctuations with periods of 20-180 days account for 50% of the variance. Bottom pressure anomaly differences provide estimates of the barotropic transport variability. Time series were calculated for 4 subregions using the pressure differences of the end points. For the NS region, the time series was calculated using the near-bottom currents which provided more continuous coverage. Standard deviation of the total barotropic transport is 18.3 Sv. Using single pressure records from the southern end misses a large fraction of the variability. The transport variability correlates better with pressures from the northern gauge. Most of the barotropic transport variability is captured by using the deepest northern gauge with any of the southern gauges as end points. cor = 0.81 C03 C16 cor = 0.76 C03 C17 cor = 0.66 C03 cor = 0.38 C16 cor = 0.24 C17 2008 2009 2010 2011 50 0 50 100 150 Total Barotropic 1. The canonical transport estimate from ISOS (Whitworth 1983; Whitworth and Peterson 1985) of 134 Sv with the revised error estimate of 27 Sv from Cunningham et al. (2003) gives a maximum transport of 161 Sv, which is in good agreement with the cDrake minimum estimate of 162 Sv. 2. Using a 4.5 year time series of directly-measured SADCP velocity data across Drake Passage, Firing et al. (2011) estimated the mean transport in the upper 1000 m of 95 ± 2 Sv. The ISOS array lost 2 critical moorings in the high transport region of the SAF and PF which would result in the transport being underestimated. A mean reference velocity of 0.04 m s -1 in this 125 km region could account for an additional 20 Sv of transport. For cDrake the baroclinic and barotropic contributions in the upper 1000 m are 77 ± 4.4 Sv and 11 ± 2.2 Sv, respectively. These combine to give a total of 88 ± 5 Sv, which is in good agreement with the Firing et al. estimate. cDrake mean transports can be compared to mean values from other time series in Drake Passage: cDrake Objectives: Determine horizontal and vertical structure of time-varying transport. Describe the mesoscale eddy field. Provide guidance for future monitoring. Assess the skill of model simulations. depth (m) 5000 4000 3000 2000 1000 0 C01 C02 C03 C04 C05 C06 C07 C08 C09 C10 C11 C12 C13 C14 C15 C16 C17 C19 C20 64 o W 62 o W 60 o W 62 o S 60 o S 58 o S 56 o S M01 M02 M03 64 o W 62 o W 60 o W 62 o S 60 o S 58 o S 56 o S H01 H02 H04 H05 H03 C10 24’ 12’ 63 o W 48’ 36’ 32’ 28’ 58 o S 24.00’ 20’ 16’ 10 3 10 2 10 1 10 0 0 50 100 150 200 250 300 Frequency (cpd) Power spectrum (Sv 2 ) Total SS NDP l l l 0.1 0 0.1 0 20 40 60 80 100 C17 M03 C16 C15 Distance (km) SS 0.1 0 0.1 360 380 400 420 440 460 C11 H01 C10 H02 H03 C09 Line normal velocity (m s 2 ) SFZ C17 M03 C16 C15 C14 C13 C12 C11 C10 C09 C08 C07 C06 C19 C05 C20 C04 C03 M02 C02 M01 C01 C17 M03 C16 C15 C14 C13 C12 C11 C10 C09 C08 C07 C06 C19 C05 C20 C04 C03 M02 C02 M01 C01 Correlation 1 0.5 0 0.5 1 20 0 20 40 60 Transport (Sv) SS SDP SFZ NDP NS SACCF PF SAF SouthtoNorth Distance (km) Depth (m) 0 100 200 300 400 500 600 700 800 0 2000 4000 90 dlp currents 3 dlp pressures

Upload: others

Post on 18-Feb-2021

2 views

Category:

Documents


0 download

TRANSCRIPT

  • 2.Mean  barotropic  transport  calculated  from  near-‐bo6om  currents  

    5.  Discussion

    Karen  L.  Tracey,  Kathleen  A.  Donohue,  and  D.  Randolph  Wa8s  

    950  

    1.  cDrake  experiment  

    [email protected]                      www.cDrake.org  

    3.  Barotropic  transport  variability  calculated  from  bo6om  pressures  

    References  Chidichimo et al. 2014. Baroclinic transport time series of the Antarctic Circumpolar Current in Drake Passage. J. Phys. Oceanogr. (submitted). Cunningham et al. 2003. Transport of the Antarctic Circumpolar Current in Drake Passage. J. Geophys. Res. 108: 8084. Firing et al. 2011. Vertical structure and transport of the Antarctic Circumpolar Current in Drake Passage from direct velocity measurements. J. Geophys. Res. 116: C08015. Koshlyakov et al. 2012. Currents in Drake Passage based on observations in November of 2010. Oceanology. 52: 299-308. Mazloff et al. 2010. An eddy-permitting Southern Ocean State Estimate. J. Phys. Oceanogr. 40: 880-899. Whitworth. 1983. Monitoring the transport of the Antarctic Circumpolar Current at Drake Passage. J. Phys. Oceanogr. 13: 2045-2057. Whitworth and Peterson. 1985.Volume transport of the Antarctic Circumpolar Current from bottom pressure measurements. J. Phys. Oceanogr. 15: 810-816.

    C17

    C16

    C15

    C14

    C13

    C12

    C11

    C10

    C09

    C08

    C07

    C06

    C19

    C05

    C20

    C04

    C03

    C02

    C01

    C17C16C15C14C13C12C11C10C09C08C07C06C19C05C20C04C03C02C01

    Correlation

    0 0.5 1

    Barotropic  Transport  of  the  AntarcDc  Circumpolar  Current  Measured  in  Drake  Passage  

     Region  

    Mean  (Sv)  

    NS   7.5          (a)  

    NDP   7.7          (a)  

    SFZ   15.9      (b)  

    SDP   15.1      (a)  

    SS   -‐2.3        (c)  

    Total   43.8  

    Visit other cDrake posters: 951 Foppert et al. Mean baroclinic structure of Polar Front in stream coordinates near Shackleton Fracture Zone. 849 Millar et al. Four-year observations of interfacial form stress in the northern Drake Passage.

    Energetic transport fluctuations with periods of 50-180 days in SFZ and NDP regions are associated with the main ACC fronts shifting between regions. These fluctuations are nearly equal and opposite, and the variability of total barotropic transport in that period band is reduced. Transport fluctuations with periods in the 50-180 day band are weak at the southern and northern subregions of the passage.

    C11-C17 pressures, south of the Shackleton Fracture Zone, exhibit less variance than those north of the topographic ridge. Southern pressure records (C17-C11) are highly correlated with one another.

    •  4-year observational period from Nov 2007 to Nov 2011.

    •  42 Current and Pressure recording Inverted Echo Sounders (CPIES) in transport line (solid triangles) and local dynamics array (open triangles).

    •  C01-C08 spacing: ~30 km •  C08-C17 spacing: ~60 km •  5 closely-spaced CPIES (H01-

    H05) along Shackleton Fracture Zone in year 4.

    •  3 short current meter moorings (M01-M03) deployed at continental margins for first 2 years.

    Bo8om  pressures  

    C01

    C02

    C03

    C04

    C20

    C05

    C19

    C06

    C07

    2008 2009 2010 2011−0.2

    00.2 C08

    C09

    C10

    C11

    C12

    C13

    C14

    C15

    C16

    2008 2009 2010 2011

    C17

    •  Leveled and dedrifted using near-bottom currents. •  Unresolved residual drift (< 1 cm per 1000 days) corresponds

    to 4 Sv barotropic transport error over a 4-year experiment.

    Line-‐normal  currents  

    dbar  

    •  Measured 50 m above the seafloor. •  Rotated to be perpendicular to the transport line.

    3 dlp currents are poorly correlated from site to site, while neighboring 90 dlp currents are positively or negatively correlated.

    All  measurements:  •  1 hour sampling interval. •  Tides removed: Semi-diurnal and diurnal

    using response analysis, fortnightly and lunar monthly tides with TPXO7.2.

    •  3 day low-pass filter applied to hourly samples and subsampled to twice daily.

    dept

    h (m

    )

    −5000

    −4000

    −3000

    −2000

    −1000

    0

    64oW 62oW 60oW

    62oS

    60oS

    58oS

    56oS

    10 cm s−1

    64oW 62oW 60oW

    62oS

    60oS

    58oS

    56oS

    dept

    h (m

    )

    −5000

    −4000

    −3000

    −2000

    −1000

    0

    64oW 62oW 60oW

    62oS

    60oS

    58oS

    56oS

    SS

    SDP

    SFZ

    NDP

    NS

    0.1 m s−1

    64oW 62oW 60oW

    62oS

    60oS

    58oS

    56oS

    Annual means are remarkably stable from year to year across the whole Drake Passage. This permits variable-record-length means to be used to estimate the barotropic transport and its error.

    The across-passage mean currents are well resolved by the closely-spaced cDrake array. Standard error ellipses are small compared to the record-length mean currents.

    Gray contours: 4-year mean SSH from Aviso (c.i. 10 cm).

    (a) Standard trapezoidal integration. (b) Distance-weighted trapezoidal integration with l = 15 km for H01 and H03. Error estimation allowed l  (distance from the Shackleton Fracture Zone) to vary between 10, 15, and 20 km based on LADCP casts taken on cDrake cruises and by Koshlyakov et al. (2012). (c) Distance-weighted trapezoidal integration with l = 24 km for C16. Error estimation was based on l  =  24  km (distance from the South Shetland Trench) and l  =  36 km (no distance weighting).

    4.  Total  transport  through  Drake  Passage  

    6.  Summary  

    −0.2

    −0.1

    0

    0.1

    0.2

    Line

    nor

    mal

    vel

    ocity

    (m s−1

    )

    C17

    M03

    C16

    C15

    C14

    C13

    C11

    C10

    C09

    C08

    C07

    C06

    C19

    C05

    C20

    C04

    C03

    M02

    C02

    M01

    C01

    yr 1yr 2yr 3yr 44 yrs

    62°S 60°S 58°S 56°S

    0

    2000

    4000Dep

    th (m

    )

    Error  EsDmaDon   Transport    (Sv)  

    Array-‐wide  resoluJon  for  90  day  low-‐passed  currents   7.7  

    CorrelaJon  scales  near  topography  in  subregion  SFZ  (b)   2.8  

    CorrelaJon  scales  near  topography  in  subregion  SS  (c)   1.8  

    Possible  bo8om  trapping  bias  (under  invesJgaJon)   -‐4  ±  4  

    Total   9.3    

    Barotropic transport is calculated using trapezoidal integration of the near-bottom velocity times the site-dependent water depth. The average site depth in the deep passage is about 4000 meters. Five subregions were defined based on topographic features: Northern and Southern Slopes (NS and SS), Shackleton Fracture Zone (SFZ), and Northern and Southern Deep Passages (NDP and SDP). H01-H03 sites were shifted along topography to the transport line to resolve the deep flow near the Shackleton Fracture Zone. The mean eastward transport accumulates beneath the SAF and PF. The mean eastward barotropic transport is 43.8 Sv with an uncertainty of 9.3 Sv. This mean transport translates to a mean across-passage eastward bottom-reference velocity of 1.3 cm s-1.

    The cDrake moored array provided measurements across the Drake Passage with high spatial and temporal resolution for four years. Annual mean currents are remarkably stable from year to year and provide robust estimates of the barotropic transport. The mean barotropic transport is 43.8 Sv ± 9.3 Sv. Variability of the barotropic transport is dominated by the variability northward and downstream of the Shackleton Fracture Zone. Summing the barotropic transport with the bottom-referenced baroclinic transport of 127.7 Sv gives a total mean eastward transport of 171.4 Sv through Drake Passage. The variability of the barotopic component accounts for the largest fraction (80%) of the total transport variability. cDrake observations have been assimilated into the Southern Ocean State Estimate (Mazloff et al. 2010). This effort will provide perspective on how the cDrake measurements and derived quantities fit into the context of local, regional and large-scale variability, and their associated forcing.

    C01

    M01

    C02

    M02

    C03

    C04

    C20

    2008 2009 2010 2011−0.4

    00.4

    m s−1 C05

    C19

    C06

    C07

    C08

    C09

    C10

    C11

    2008 2009 2010 2011

    C12

    C13

    C14

    C15

    C16

    M03

    2008 2009 2010 2011

    C17

       

    Record-length mean near-bottom currents perpendicular to the transport line were used to determine the mean barotropic transport.

    J A J O J A J O J A J O J A J O

    SS

    SDP

    SFZ

    NDP

    NS

    Total Barotropic

    50 S

    v

    2008 2009 2010 2011

    3 dlp and 90 dlp Transports By Region

    Transports            (Sv)  

    4  year  Mean  

    SEM    

    Std  dev  

    Yr    1  Mean  

    Yr  2  Mean  

    Yr  3  Mean  

    Yr  4  Mean  

    Baroclinic  +  Barotropic  

    171.4   3.1   18.7   170.1   175.8   177.2   162.7  

    Baroclinic   127.7       1.0      8.1   128.0   128.5   126.8   127.4  

    Barotropic      43.8         3.0   18.3   42.2   47.3   50.4   35.3  

    J A J O J A J O J A J O J A J O−50

    0

    50

    100

    150

    200

    250Baroclinic + Barotropic

    Baroclinic

    Barotropic

    Tran

    spor

    t (Sv

    )2008 2009 2010 2011

    Full-depth baroclinic transport referenced to zero at the bottom was calculated from the cDrake CPIES records by Chidichimo et al. (2014).

    While the barotropic component accounts for only 25% of the total transport, with a temporal standard deviation of 18.3 Sv, it accounts for 80% of the total variability observed over the four years.

    NSF Office of Polar Programs supported this work under grants ANT-0635437 and ANT-1141802.

    Steady annual mean transports confirm that the 4-year means are robust.

    Baroclinic component of 127.7 Sv accounts for 75% of the total eastward transport of 171.4 Sv through Drake Passage.

    Transport fluctuations with periods of 20-180 days account for 50% of the variance.

    Bottom pressure anomaly differences provide estimates of the barotropic transport variability. Time series were calculated for 4 subregions using the pressure differences of the end points. For the NS region, the time series was calculated using the near-bottom currents which provided more continuous coverage.

    Standard deviation of the total barotropic transport is 18.3 Sv.

    Using single pressure records from the southern end misses a large fraction of the variability.

    The transport variability correlates better with pressures from the northern gauge.

    Most of the barotropic transport variability is captured by using the deepest northern gauge with any of the southern gauges as end points.

    cor = 0.81 C03 − C16

    cor = 0.76 C03 − C17

    cor = 0.66 C03

    cor = −0.38 C16

    cor = −0.24 C17

    2008 2009 2010 2011−50

    050

    100150 Total Barotropic

    1.  The canonical transport estimate from ISOS (Whitworth 1983; Whitworth and Peterson 1985) of 134 Sv with the revised error estimate of 27 Sv from Cunningham et al. (2003) gives a maximum transport of 161 Sv, which is in good agreement with the cDrake minimum estimate of 162 Sv.

    2.  Using a 4.5 year time series of directly-measured SADCP velocity data across Drake Passage, Firing et al. (2011) estimated the mean transport in the upper 1000 m of 95 ± 2 Sv.

    The ISOS array lost 2 critical moorings in the high transport region of the SAF and PF which would result in the transport being underestimated. A mean reference velocity of 0.04 m s-1 in this 125 km region could account for an additional 20 Sv of transport.

    For cDrake the baroclinic and barotropic contributions in the upper 1000 m are 77 ± 4.4 Sv and 11 ± 2.2 Sv, respectively. These combine to give a total of 88 ± 5 Sv, which is in good agreement with the Firing et al. estimate.

    cDrake mean transports can be compared to mean values from other time series in Drake Passage:

    cDrake Objectives: •  Determine horizontal and vertical structure of time-varying transport. •  Describe the mesoscale eddy field. •  Provide guidance for future monitoring. •  Assess the skill of model simulations.

    dept

    h (m

    )

    −5000

    −4000

    −3000

    −2000

    −1000

    0

    C01C02C03C04C05

    C06C07C08

    C09

    C10

    C11

    C12

    C13

    C14C15

    C16

    C17

    C19

    C20

    64oW 62oW 60oW

    62oS

    60oS

    58oS

    56oS

    M01M02

    M03

    64oW 62oW 60oW

    62oS

    60oS

    58oS

    56oS

    H01H02

    H04H05 H03

    C10 24’ 12’

    63oW 48’ 36’

    32’ 28’

    58oS 24.00’

    20’ 16’

    10−3 10−2 10−1 1000

    50

    100

    150

    200

    250

    300

    Frequency (cpd)

    Pow

    er s

    pect

    rum

    (Sv2

    )

    TotalSSNDP

    l

    l

    l

    −0.1 0 0.1

    0

    20

    40

    60

    80

    100

    C17

    M03C16

    C15

    Dis

    tanc

    e (k

    m)

    SS

    −0.1 0 0.1

    360

    380

    400

    420

    440

    460

    C11

    H01C10

    H02H03

    C09

    Line normal velocity (m s−2)

    SFZ

    C17

    M03

    C16

    C15

    C14

    C13

    C12

    C11

    C10

    C09

    C08

    C07

    C06

    C19

    C05

    C20

    C04

    C03

    M02

    C02

    M01

    C01

    C17M03C16C15C14C13C12C11C10C09C08C07C06C19C05C20C04C03M02C02M01C01

    Correlation

    −1 −0.5 0 0.5 1

    −20

    0

    20

    40

    60Tr

    ansp

    ort (

    Sv)

    SS SDP SFZ NDP NS

    SACCF PF SAF

    South−to−North Distance (km)

    Dep

    th (m

    )

    0 100 200 300 400 500 600 700 800

    0

    2000

    4000

    90 dlp currents

    3 dlp pressures