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Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA 93106

Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

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Page 1: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Ocean Surface Current Observations in PWS

Carter Ohlmann

Institute for Computational Earth System Science, University of California, Santa Barbara, CA 93106

Page 2: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

ROMS-based dispersal simulationROMS-based dispersal simulation

Deployment sites have 5 km radius and are adjacent to the coast

From each site, around 100 particles are released every 12 hours from Jan. 1996 – Dec. 2002

Lagrangian PDFs are calculated for 1 – 14 day advection times

PDFs = probability density functions

Page 3: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Drifter dataDrifter data (CODE 1 meter; MMS SBC-SMB (CODE 1 meter; MMS SBC-SMB study)study)

SCB drifter data on the regional scale

Drifters deployed ~ quarterly from 1993 – 1999. 568 drifters sampling for an average of ~24 days give ~13,500 drifter days of data.

Drifter dispersal from a single site

Red circle: “release” site

Blue dots: drifter locations for a give advection time

Page 4: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Lagrangian PDF vs Drifter Lagrangian PDF vs Drifter DistributionDistribution

Drifter locationsDrifter locations

Page 5: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Project Goal: Provide improved real-time ocean current and wind forecasts with error estimates for inclusion in USGC DSTs.

Pathway to Project Goal:• Benchmark DSTs (year 1)

• Develop and evaluate improved data assimilating models (year 2)

Page 6: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

24 hrs

1000 m

100 m

10 m

Motivation for this research component:

Benchmarking, evaluating, and assimilating data into DSTs (focused on transport pathways) requires a thorough understanding of surface current observations.

Data from drifting buoys are key as drifters provide direct observations of both advection and diffusion, the two processes responsible for defining a search area.

Page 7: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Outline:• Instrumentation for measuring ocean surface currents- HF radar derived surface currents- Drifting buoys- SLDMBs

• Ocean surface current data collected during year 1 field program- 54 drifter tracks w/ 12 drifters

• Preliminary analysis of year 1 surface current data- SLDMB performance- HF radar “ground truth”

• Work plan for year 2

Page 8: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Microstar Drifters:• tri-star drogue centered at 1 m depth

• 10 minute position sampling w/ GPS

• data transmission through Iridium

• 1 cm/s slip in 10 m/s wind

• 7 day life expectancy

• real time data on web

• recoverable

Ohlmann et al. 2005, and Ohlmann et al. 2007

www.drifterdata.com

Page 9: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Microstar drifter data during PWS FE:

• 12 drifters used; 12 drifters worked; 1 drifter lost

• 54 drifter trajectories sampled

• mostly ~2 days in length

• positions every 10 minutes

Page 10: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

USCG SLDMB• marker buoy used by USCG

• based on 1970’s design

• altered dimensions

•water-following characteristics not found in scientific literature

• 30 minute position data

• data transmission: Argos

• difficult to recover

Page 11: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

USCG SLDMB data during PWS FE: • 9 drifters used; 8 drifters worked; 9 drifters lost

• 8 drifter trajectories sampled

• mostly numerous days in length

• positions every 30 minutes

Page 12: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

HF radar surface currents – Bragg scattering off surface gravity waves with known wavelength, extract wave speed, get surface current.Typically 15 – 30 minute averages reported hourly for a 1 – 10 km grid.

Velocity “errors” of 10 cm/s typically quoted

Page 13: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

HF radar surface currents – time-space (1 hr - 1 km) average surface current maps such as this were produced throughout the PWS FE (~14 days).

PWS HF radar locations

Page 14: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

PWS HF radar surface current map – spatial extent of coverage is highly variable.

PWS HF radar locations

Page 15: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

starting positions

ending positions

USCG SLDMBsMicrostar drifters

Preliminary analysis of data:

Q: What can be learned of SLDMB water-following capabilities?

Page 16: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Preliminary analysis of data:

A: SLDMBs move ~1.0 cm/s slower.

~400 m separation after ~18 hours

advection difference

diffusion differencesimilar diffusion characteristics for first 19 hours

Page 17: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Preliminary analysis of data:

Ocean turbulence, u’(x,y,t), complicates comparative analyses.

starting positions

ending positions

USCG SLDMBsMicrostar drifters

Page 18: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Preliminary analysis of data:

A: SLDMBs move ~3 – 4 cm/s “differently”. Need to understand why?

~8000 m separation after ~55 hours

advection difference

diffusion difference

similar diffusion characteristics

Page 19: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Preliminary analysis of data:

Q: How well do drifter and HF radar observations agree?

7 HF radar radial cells

20 drifter tracks

Need to compute time-space averages from drifter clusters for HF radar ground truth.

Page 20: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Preliminary analysis of data:

Q: How well do drifter and HF radar observations agree?

14 HF radar radial cells

20 drifter tracks

Need to compute time-space averages from drifter clusters for HF radar ground truth.

Page 21: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Preliminary analysis of data:

Q: How well do drifter and HF radar observations agree?

HF radar velocities show large variance on few km space scales

> 70 cm/s range

Page 22: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Preliminary analysis of data:

Q: How well do drifter and HF radar observations agree?

HF radar velocities show large variance on few km space scales

> 40 cm/s range

Page 23: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Preliminary analysis of data:

Looking at a single radial cell comparison.

> 25 cm/s difference between drifter and HF radar derived surface velocities

Page 24: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Preliminary analysis of data:

Looking at a single radial cell comparison.

drifter and HF radar velocities agree to within a few cm/s

> 40 cm/s difference between drifter and HF radar derived surface velocities

Page 25: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Summary:

Year 1 accomplishments

• Successful field experiment. 12 drifters were used to sample 54 drifter tracks, only 1 drifter lost

• First set of coincident SLDMB and drifter observations

• Observations for evaluating HF radar surface currents

Year 2 workplan

• SLDMB performance analysis with wind data

• HF radar ground truth analysis

• Benchmark for ROMS simulations

• Quantify parameters for a PWS Lagrangian Stochastic Model

Page 26: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA
Page 27: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

exponential growth during first 4 hours

Mean Dispersion Values:

D2(t) = exp(At) ; A-1 = 60 min ; r2 = 0.911000 m

100 m

10 m

Page 28: Ocean Surface Current Observations in PWS Carter Ohlmann Institute for Computational Earth System Science, University of California, Santa Barbara, CA

Definitions:

Relative Dispersion

• Spread (or variance) of a set of particles relative to coordinate

frame fixed to the cloud’s center of mass (“two particle” statistics)

Eddy Diffusivity

• Time rate of change of dispersion

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