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Ocean Modeling Requirements for Decadal-to-Centennial Climate

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Dec-Cen Climate is Operational, but not in Real Time. ... Wall-clock model speeds are 103-104 ... Beckman & Doscher (JPO 1997), Campin & Goose (Tellus 1999) ... – PowerPoint PPT presentation

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Title: Ocean Modeling Requirements for Decadal-to-Centennial Climate


1
Ocean Modeling Requirementsfor
Decadal-to-Centennial Climate
  • Robert Hallberg
  • NOAA/GFDL

2
Ocean Modeling Considerationsfor
Decadal-Centennial Climate
  • Dec-Cen Climate is Operational, but not in Real
    Time.
  • Ocean models are fully global and must include
    sea-ice.
  • Models run for O(1000-year) timescales.
  • Wall-clock model speeds are 103-104 times real
    time.
  • Ocean biases after a spinup of hundreds of years
    must be acceptably small.
  • Data assimilation during the run or unphysical
    damping are unacceptable in Dec-Cen climate
    models.
  • Precise initial values are often relatively
    unimportant.
  • The long timescales mean that a wide range of
    physical processes must be represented as
    credibly as possible.

3
Ocean Climate Models must be Conservative.
  • Non-conservation leads to drift and uncertainty.
  • Tolerances for non-conservation
  • Mass small compared to sea-level rise.
  • 20th Century rise 10 cm.
  • Err ltlt 10-3 m cen-1 MOM, GOLD 10-7 m cen-1
  • Heat small compared to anthropogenic forcing
  • Anomalous Radiative Forcing 4 W m-2 at CO2
    doubling
  • Err ltlt 0.1 W m-2 MOM, GOLD 3x10-6 W m-2
  • Total Salt small compared to sea-level rise
    dilution?
  • Dilution of Salinity 10-3 PSU cen-1
  • Err ltlt 10-4 PSU cen-1 MOM, GOLD 3x10-9 PSU
    cen-1
  • With care, these tolerances can be achieved in
    all classes of ocean models. (MOM Z-coord., GOLD
    r-coord.)

4
Key Metrics of a Global Ocean Climate Model
  • SST biases at equilibrium
  • ENSO statistics (Amplitude Frequency) at
    equilibrium
  • Tropical ocean circulation and watermass
    structure at equilibrium.
  • Stability and strength of meridional overturning
    circulation and gyre circulations.
  • (Important for meridional heat transport
    sea-ice distribution)
  • Equilibrium watermass properties, rates and
    processes of formation destruction.
  • (Important for storage of heat, carbon, etc.)
  • Spurious diapycnal mixing ltlt physical Kd 10-5
    to 10-6 m2 s-1
  • Overflows entraining gravity currents
  • Mode-water formation processes

5
100-year-mean SST Biases in GFDLs CM2.1 Coupled
Climate Model
6
Equatorial Pacific Velocities and Temperatures
after 500 years in CORE simulations with 7 models
Drifts accumulate over 50 years. Short runs may
not be indicative of equilibrium climate.
(Figs. from Griffies et al., Ocean Mod., Sub.)
7
Challenges in Global Ocean Climate Modeling
  • Increasing resolution to admit mesoscale eddies

8
Role of eddies in Southern Ocean Dynamics
  • Eddies alter the sensitivity to forcing changes
    of the Southern Ocean overturning circulation and
    the resultant ventilation of the interior ocean.

Hallberg Gnanadesikan, JPO 2006
9
Challenges in Global Ocean Climate Modeling
  • Increasing resolution to admit mesoscale eddies
  • Dramatic increase in model cost, reduction in
    speed
  • Changes in required parameterizations
  • Numerical constraints (e.g. on spurious diapycnal
    mixing) become harder to satisfy.
  • Regional climate impacts

10
SST in a Prototype 1/8 Global Ocean Model
Upwelling zone
California Current
11 Box Contemporary Climate Model Resolution
11
Challenges in Global Ocean Climate Modeling
  • Increasing resolution to admit mesoscale eddies
  • Dramatic increase in model cost, reduction in
    speed
  • Changes in required parameterizations
  • Numerical constraints (e.g. on spurious diapycnal
    mixing) become harder to satisfy.
  • Regional climate impacts
  • Dominant scales of many ecosystems much smaller
    than well-resolved by global physical climate
    models.
  • Two-way nesting is probably needed.

12
The Existing GFDL Suite of Ocean Models
  • GFDL/Princeton has leading developers of each
    widely used class of large-scale ocean models.
  • MOM B-grid Z-coordinate model
  • MITgcm C-grid Z-coordinate model with
    nonhydrostatic capabilities
  • HIM C-grid isopycnal coordinate model
  • POM Princeton AOS programs C-grid sigma
    coordinate model
  • The Generalized Ocean Layer Dynamics (GOLD)
    ocean model unites the GFDL efforts.
  • GOLD is an ocean modeling system that combines
    the capabilities of GFDLs MOM and HIM and the
    MITgcm ocean models into a single flexible
    code-base.
  • GOLD numerics will be suitable for studying
    climate, but with demonstrated proficiency for a
    variety of other applications (tides,
    nonhydrostatic mixing, etc.)
  • GOLD will include significant nesting and data
    assimilation capabilities.
  • GFDL ocean models focus on integrity for climate
    applications.

Developers at GFDL/Princeton
13
GOLD and HYCOM
  • GOLD is structurally compatible with HYCOM.
  • The GOLD dynamic core overall structure are
    derived from the isopycnal coordinate model HIM.
    Similar issues must be addressed as for HYCOM.
  • GOLD has necessary qualities for long-term
    climate studies.
  • Conservation-to-roundoff of heat, salt, mass, and
    tracers.
  • Accurate with a fully nonlinear equation of
    state.
  • Robust parameterizations of small-scale
    processes.
  • Rotated diffusion tensor minimized spurious
    diapycnal mixing.
  • An NSF-funded project, including GOLD, HYCOM and
    ROMS, is exploring standardization across ocean
    models.
  • Collaborations are welcomed, provided they do not
    disrupt GFDLs primary mission in long-term
    climate studies.

GOLD
?
z
z/z/p/p
HIM
Poseidon
HyCOM
MOM
MITgcm
POP
14
Potential for One NOAA Ocean Model Addressing
Real-time Operational Global Dec-Cen Climate
  • What is a model?
  • A single model configuration.
  • Unlikely, due to mismatch in timescales, model
    speed, emphasis on initial conditions vs. bias.
  • A shared model code-base.
  • Repository of best theories/techniques for both
    real-time operations and climate. Natural
    synergies could emerge.
  • Will take considerable work and resources.
  • Important not to disrupt the on-going operational
    requirements for real-time forecasts or climate.
  • Establishing common model interfaces would be a
    natural first step.
  • Some ocean forecasting applications (e.g.,
    tsunami warnings) are so different that they are
    unlikely ever to use the same model.

15
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16
High-Resolution Ocean Modeling the Ocean
Research Priorities Plan
  • Numerical ocean models are recognized as crucial
    tools for a wide range of questions (ORPP, p.
    47).
  • High resolution global ocean modeling is central
    to the ORPPs Theme 4 The Oceans Role in
    Climate and the near-term priority Assessing
    Meridional Overturning Circulation Variability
  • Resolving the critical processes is crucial for
    reducing the uncertainty in projections.
  • The insight gained from the Global Ocean
    Observing System is maximized when the data is
    interpreted in the context of numerical models.
  • High resolution global ocean simulations are
    valuable in support of the other 5 Themes.
  • Provide consistent boundary conditions for
    ultrafine regional models.
  • Provide estimates of variability in the
    conditions faced by ecosystems, marine
    operations, or processes affecting human health.
  • NOAA/GFDL is taking the lead in addressing the
    ORPP call for a coherent, comprehensive global
    modeling capability, addressing Theme 4 in
    particular.

17
Mean Salinity Drifts in 7 CORE Forced Candidate
Ocean Climate models (Griffies et al., 2008)
Notes Sea-ice growth is the sole cause of
salinity drift in some models. Some
models balance salinity restoring, others do not.
18
Frontal Dynamics and Resolution
  • Upwelling jets fronts require higher
    resolutions than current ocean climate models.
  • With steady forcing all variability is due to
    ocean dynamics.

Hallberg Gnanadesikan, JPO 2006
19
Strengths and Weaknesses of Terrain-following
Coordinate Models
  • (Issues for global climate application addressed
    in detail by G. Danabasoglu later.)
  • Strengths
  • Topography is represented very simply and
    accurately
  • Easy to enhance resolution near surface.
  • Lots of experience with atmospheric modeling to
    draw upon.
  • Traditional Weaknesses
  • Pressure gradient errors are a persistent
    problem.
  • Errors are reduced with better numerics (e.g.,
    Shchepetkin McWilliams, 2003)
  • Gentle slopes (smoothed topography) must be used
    for consistency
  • Traditional requirement for stability (Beckman
    Haidvogel, 1993)
  • ROMS requirement (Shchepetkin, pers. comm)
  • Spurious diapycnal mixing due to advection may be
    very large. (Same issue as Z-coord.)
  • Diffusion tensors may be especially difficult to
    rotate into the neutral direction.
  • Strongly slopes require larger vertical stencil
    for the isoneutral-diffusion operator.

20
Resolution requirements for avoiding numerical
entrainment in descending gravity currents.
  • Z-coordinate
  • Require that
  • AND
  • to avoid numerical entrainment.
  • (Winton, et al., JPO 1998)
  • Many suggested solutions for Z-coordinate models
  • "Plumbing" parameterization of downslope flow
  • Beckman Doscher (JPO 1997), Campin Goose
    (Tellus 1999).
  • Adding a separate, resolved, terrain-following
    boundary layer
  • Gnanadesikan (1998), Killworth Edwards (JPO
    1999), Song Chao (JAOT 2000).
  • Add a nested high-resolution model in key
    locations?
  • Sigma-coordinate Avoiding entrainment requires
    that
  • But hydrostatic consistency requires
  • Isopycnal-coordinate Numerical entrainment is
    not an issue - BUT
  • If resolution is inadequate, no entrainment can
    occur. Need

21
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22
Horizontal Resolution (in km) Required to Permit
50m Vertical Resolution at Bottom
23
Horizontal Resolution (in km) Required to Permit
50m Vertical Resolution at Bottom
24
Horizontal Resolution (in km) Required to Permit
50m Vertical Resolution at Bottom
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