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EVALUATION OF UPPER OCEAN MIXING PARAMETERIZATIONS

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EVALUATION OF UPPER OCEAN MIXING PARAMETERIZATIONS. S. Daniel Jacob1, Lynn K. ... Hycom Q Movie. Gaspar. MY2.5. KPP. PWP. 2 Rmax. No Precip. Precip. Objectives ... – PowerPoint PPT presentation

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Title: EVALUATION OF UPPER OCEAN MIXING PARAMETERIZATIONS


1
EVALUATION OF UPPER OCEAN MIXING PARAMETERIZATIONS
  • S. Daniel Jacob1, Lynn K. Shay2 and George R.
    Halliwell2

1 GEST, UMBC/ NASA GSFC, Greenbelt, MD 20771 2
MPO, RSMAS, University of Miami, Miami, FL 33149
Alan Wallcraft (NRL Stennis) Chet Koblinsky (NOAA)
2
Importance of Ocean Mixing
  • Based on Observational Analysis (Jacob et al.,
    JPO 2000)
  • Entrainment is the dominant mechanism in
    controlling mixed layer budgets.
  • Mixed layer heat and mass budgets strongly depend
    upon the entrainment scheme used crucial for
    intensity prediction.
  • Numerical Modeling (Jacob and Shay, JPO, 2003)
  • Measured and simulated quantities based on
    different hypothesis are used to compute
    entrainment mixing.
  • Bulk schemes in MICOM also indicated strong flux
    variability.

3
Motivation HYbrid Coordinate Ocean Model (HYCOM)
Results
(Bleck 2002, Halliwell 2004)
  • Configuration
  • Domain Gulf of Mexico
  • Resolution 0.07?
  • 50 Levels/ Layers
  • Closed Boundaries
  • Initial Conditions
  • Quiescent Conditions with Gilbert forcing
  • SST Variability
  • Significant in the directly forced region
  • Large range in fluxes
  • Sensitivity to precipitation

4
Hycom Q Movie
Gaspar
KPP
MY2.5
PWP
5
2 Rmax
No Precip
Precip
6
Objectives
  • Evaluate and Validate Mixing Schemes to identify
    the most appropriate parameterizations for use in
    coupled prediction model.
  • Schemes in the Hybrid Coordinate Ocean Model
  • K Profile Parameterization (Large et al. 1994
    KPP)
  • Gaspar (1988)
  • Price et al. (1986 PWP) scheme.
  • Mellor and Yamada (1974 MY2.5) Level 2.5 K-e
    scheme
  • Canuto et al. (2001, 2002 GISS)
  • Compare Simulations to Observations
  • Gilbert (1988)
  • Isidore (2002)
  • Lili (2002)

7
Project Schedule
  • Model Configuration, set up, derivation of
    initial conditions and forcing February 2004.
  • Gilbert simulations and comparison May 2004
  • Isidore and Lili Simulations and comparison to
    observations Jan 2005
  • Recommendation of the most appropriate mixing
    scheme for use in coupled prediction models. Aug
    2005.

8
Model Configurations
  • Gilbert (1988)
  • Prior HYCOM/ MICOM configuration on Mercator grid
    at 0.07 resolution at the equator.
  • Buffer zones at open boundaries relaxed to
    climatology.
  • Simulations from 14 Sep 1988 to 20 Sep 1988.
  • Isidore (2002) and Lili (2002)
  • Domain includes Caribbean Sea and the Gulf of
    Mexico.
  • Treated as a single case with 20 day integration
    for each mixing parameterization.
  • Configured as a nest of the basin scale HYCOM
    that provides conditions at the open boundaries.

9
Gilbert Initial Conditions
  • Pre-storm variability due to a Loop Current Warm
    Core Eddy (LCWCE) Eddy F
  • Sampled extensively by Minerals Management
    Service - Yearday 200/300 data.
  • Propagated westward at 3 to 4 km/day (Average
    translation speed 5 km/day for Gulf eddies
    Vukovich and Crissman 1986).
  • Possess distinct T-S relationship corresponding
    to the subtropical water mass. Shay et al.
    (1998) derived the T-S relationship for the Gulf
    Common Water and the Loop Current Eddy Water
    using historical and Yearday 200/300 data set.
  • Realistic initial conditions are derived by
    combining the objectively analyzed day 200 data
    with the Levitus climatology.

10
Temperature-Salinity Diagram
LCW
GCW
11
Pre-Gilbert Sea Surface Height
  • HYCOM is initialized following the methodology
    used by Jacob and Shay (2003).
  • Location of pre-storm eddy (LCWCE F) is
    accurately reproduced.
  • Depth of 26 C and 20 C isotherms compare well
    to observations.

12
Isidore Initial Conditions
  • Pre-storm variability due to the Loop Current in
    the Eastern Gulf of Mexico.
  • As the source of eddies, the Loop Current Water
    possess the same distinct T-S relationship
    corresponding to the subtropical water mass.
  • Realistic initial conditions from the 0.08 North
    Atlantic HYCOM. Courtesy of the Data Assimilative
    Ocean Modeling NOPP project of RSMAS, University
    of Miami and Naval Research Lab, Stennis Space
    Center.
  • The location of boundary currents and eddies are
    reproduced accurately by the basin-scale nowcast/
    forecast system.
  • Fields evaluated with respect to expendable probe
    data.

13
Hycom Nowcast/Forecast System
(Smedstad et al. 2003)
  • North Atlantic Hycom at 0.08 resolution
    extending from 28 S to 70 N. 26 levels/ layers
    in the vertical. High resolution surface forcing
    from FNMOC with Salinity relaxation at the
    surface. 3 buffer zones in the north and south
    relaxed to climatology.
  • Satellite altimeter height anomalies from the
    MODAS operational system at NAVOCEANO.
  • Mean Sea Surface Height from the 0.08 Atlantic
    MICOM.
  • Vertical projection of surface height signature
    using the Cooper-Haines (1996) technique.
  • Sea Surface Temperature not assimilated at
    present.

14
Pre-Isidore Sea Surface Height 19 Sept 2002
  • Pre-storm mesoscale variability is accurately
    reproduced in terms of simulated SSH.
  • Corresponds to 19 Sept 2002 pre-storm experiment.

15
Sea Surface Height Anomaly and Ocean Heat Content
19 Sept 2002
16
Pre-Isidore Sea Surface Temp 19 Sept 2002
  • Pre-storm sea surface temperatures in the
    assimilated fields are biased lower throughout
    the domain with 0.5 C in the Caribbean Sea and
    slightly higher elsewhere.

17
Meridional Cross Section along 84 W
The depth of 26 and 20 C isotherms compare well
to profiler data in the Caribbean Sea.
18
Meridional Cross Section along 86 W
Due to the lower SSTs, the depth of 26 and 20 C
isotherms are shallower compared to profiler data
by 10 m on the average in the central gulf of
Mexico.
19
Zonal Cross Section along 24 N
The model captures subsurface structure
variability due to assimilated altimetric heights
well.
20
Wind Forcing
  • Gilbert (1988)
  • Flight level reduced winds and buoy data in the
    core.
  • ECMWF 6 hourly surface data provides large scale
    field.
  • Combined using NOAA Hurricane Research Division
    HWIND program to produce wind forcing every 3
    hours.
  • Constant air temperature and relative humidity
    with synthetic rain rates derived from wind field
    distribution.
  • Isidore (2002) and Lili (2002)
  • Flight level reduced winds and buoy data analyzed
    using HWIND available on regular grid (courtesy
    Dr. Mark Powell).
  • FNMOC surface forcing provides the large scale
    forcing.
  • Blended using the parameter matrix objective
    analysis technique of Mariano and Brown (1992)
    with cubic splines every 3 hours.

21
Gilbert Wind Field Structure 16 Sep 88 06UTC
The double eyewall structure is captured
accurately by the analysis
22
Lili Wind Field Structure 02 Oct 02 00UTC
The parameter matrix algorithm works well in
blending the large scale data with the HWIND
analysis.
23
Summary and Future Work
  • Initial Conditions and forcing are established to
    investigate the sensitivity of mixing
    parameterizations in upper ocean heat content
    simulations.
  • While the Gilbert initial conditions compare well
    with pre-storm observations, the SST prior to
    Isidore is biased low in the model by an RMS
    difference of 1.1 C in the domain. Updated
    fields where SSTs are assimilated will fix this
    problem for the Isidore and Lili cases. With a
    RMS differences of about about 0.2 m/s, simulated
    current field compares well with profiler data.
    Detailed comparisons are in progress to validate
    the initial fields.
  • The parameter matrix based objective analysis
    technique works well to blend the wind analysis
    data with large scale model fields. This will be
    further improved during the course of the
    project.
  • The upper ocean response during hurricane Gilbert
    will be performed in the next phase followed by
    Isidore and Lili simulations.
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