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Waves and operational oceanography : toward a

coherent description of the upper ocean

Fabrice Ardhuin, A. Jenkins, Danièle Hauser, A. Reniers, Bertrand Chapron

To cite this version:

Fabrice Ardhuin, A. Jenkins, Danièle Hauser, A. Reniers, Bertrand Chapron. Waves and operational

oceanography : toward a coherent description of the upper ocean. Eos, Transactions American

Geo-physical Union, American GeoGeo-physical Union (AGU), 2005, 86 (4) (4), pp.37-40. �hal-00142465�

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Eos, Vol. 86, No.

4,

25 January 2005

EOS, TRANSACTIONS, AMERICAN GEOPHYSICAL UNION

VOLUME 86 NUMBER 4

25 JANUARY 2005

PAGES 3 7 - 4 4

Waves and Operational

Oceanography: Toward a Coherent

Description of the Upper Ocean

PAGES 3 7 , 4 0

The availability of new operational services for o c e a n circulation modeling presents a unique opportunity to rethink the operational forecasting of o c e a n waves and how circula­ tion and waves may b e c o m b i n e d to provide a better understanding of the upper o c e a n and e n h a n c e d services to society The large-scale oil spill caused by the wreck of the tanker Prestige off the Spanish coast in November 2002, and uncertainties on the fate of that pol­ lution, illustrated the gaps in m e a n s of obser­ vations and knowledge of relevant processes.

The idea of a c o u p l e d atmosphere-waves-o c e a n matmosphere-waves-odel was pratmosphere-waves-opatmosphere-waves-osed by Klaus Hassel-mann [HasselHassel-mann, 1991],in the context of climate modeling. As waves are the "gearbox" between the atmosphere and the o c e a n , a detailed understanding of waves c a n signifi­ cantly improve the parameterization of air-sea fluxes and surface processes. Besides, Earth observation systems rely extensively on satel­ lite remote sensing techniques for surface winds, temperature, s e a level, o c e a n color, and s e a ice, all affected by surface waves. Hassel­ mann viewed the future of wave modeling as the development of this central gearbox of a general Earth observation and monitoring sys­ tem, providing fluxes between o c e a n and atmosphere in a way consistent with satellite observations.This vision, though slow to mate­ rialize, is highly relevant for short-term forecast­ ing in the coastal o c e a n .

Waves: From Global to the Near-Shore

Wave forecasting b e c a m e a s c i e n c e in the wake of the wartime efforts of H. U. Sverdrup and W H. Munk, and was greatly improved in recent years with the development of accurate global wave models. Many operational centers are now predicting waves from wind forecasts by using a spectral frequency-direction decom­ position of the wave field; this method predicts the c h a n g e of energy for every component of

B Y FARDHUIN, A . D. JENKINS, D. HAUSER, A . RENIERS, AND B . CHAPRON

this wave spectrum, which varies in s p a c e over scales from kilometers to o c e a n basins.

It is now also possible to make reliable pre­ dictions of wave breaking statistics on b e a c h e s and the induced long-shore currents. However, the forecasting of the transformation of waves over shallow continental shelves still needs to reach that s a m e level of a c c u r a c y Such an improvement would provide offshore boundary conditions to hydrodynamic models for the surf zone and for the resulting short-term sedi­ ment transport and beach erosion [Reniers et ai, 2004],Around the surf z o n e , a n important role is played by the low-frequency motions, asso­

ciated with wave groups, that are still poorly predicted.

The Case for a Combined Ocean Circulation-Wave Forecasting System

Currents, temperature, and salinity in the world o c e a n p o s e a more c o m p l e x problem b e c a u s e they are dominated by energetic small-scale ( 5 0 - 1 0 0 k m ) eddies that have internal, albeit slow, dynamics.These eddies and the large-scale currents are only indirectly forced by surface winds, heating, or cooling. However, there are clear signs of significant effects of waves on the surface temperature and currents [Mellor and Blumberg, 2004]

Existing wave models have b e e n invoked to better parameterize surface mixing and air-sea fluxes in o c e a n circulation models, and surface currents can b e used in wave models to improve forecasts, in particular for areas where danger­ ous waves are created by opposing currents. Besides these two main reasons for forcing o n e model with the other, global and regional Total wind stress xa

wind stress for mean flow xa- xm

(direct) i

wind stress for waves (wind input): x i n

wave to mean flow stress (wave dissipation): x d i s

"normal" eddy diffusion

Mixing processes

net stress to waves :x 1 1

(wave growth/decay)^ . dis

Current boundary layer ( j A z =

Depth of penetration of the Stokes drift

mixed layer depth

Drift velocity

profile U

; - <h> + 52 • <h> + 5i = - <h>

Sediments

Fig. 1. Momentum fluxes and mixing processes coupling waves and currents. Processes for hori­ zontally uniform conditions, and possible profiles of eddy viscosity and drift velocity. Original col­ or image appears at back of this volume.

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Eos, Vol. 86, No.

25 January 2005

x ( k m )

100 120

Observed roughnness converted to wind speed (m/s)

-0.6 -0.2 0.2 0.6 radiaJ scatterer velocities (m/s)

-1.2 -0.4 0.4 1.2 Radial tidal model velocity at 5 m depth (m/s)

Fig. 2. Illustration of sea-state impact on remote sensing. High-resolution information is extracted from a single synthetic aperture radar image acquired by ENVISATover the coast of Normandy and the Channel Islands in March 2003. (Left) Surface roughness (radar cross section) interpreted in terms of wind speed but partly due to currents. (Middle left) Significant wave height computed from wave spectra. (Middle right) Radial velocity, positive to the west-southwest, due to surface drift, as seen by the radar. This surface drift is well correlated with the strong tidal currents (right panel shows modeled astronomical tidal currents) in that area and likely contains the Stokes drift due to waves. SAR data were provided by ESA, and image processing was performed by Fabrice Collard, Boost Technologies, Plouzane, France. Original color image appears at back of this volume.

circulation models rely on satellite range measurement of the s e a surface height.These measurements must b e corrected for the s e a state bias, a p h e n o m e n o n mostly related to the geometry of waves, and the largest source of error for the current operational instruments. This bias could b e c o m p u t e d from a reliable model of the wave spectrum.

Wave effects also influence other observa­ tions that should b e assimilated soon into o c e a n circulation models.The remote sensing of surface salinity faces the difficult challenge of removing the first order effects of surface roughness and wave breaking, effects that also influence the interpretation of o c e a n color. From s p a c e , surface velocity c a n b e estimated using the Doppler information of synthetic aperture radars, either by interferometry with several satellite missions in planning, or by Doppler centroid analysis using today's satel­ lites. The interpretation of these velocities will require a careful understanding of wave kine­ matics.

Among other remote-sensing techniques, High Frequency radar surface velocity estimates have b e e n experimentally assimilated in cir­ culation models. However, these measurements of "drift currents" include the wave-induced Stokes drift [Broche et ai, 1983], estimated to b e 2 0 - 8 0 % of the surface drift. (Profiles of Eulerian velocity by Santala andTerray [1992] or Mellor and Blumberg [2004] c a n b e c o m ­ pared to the often used formula for the surface drift: 3% of the wind s p e e d ) .

Although this Stokes drift is important for applications such as search and rescue, or forecasting of pollution drift, it is not properly represented in "circulation-only" models. One solution could b e the assimilation of these measurements in coupled wave-circulation models that describe the full surface drift velocity

It is All One Single Ocean

R e c e n t works by specialists in o c e a n circu­ lation modeling [e.g.,Mellor, 2003] attempt to

look at wave effects on circulation and mixing. These efforts should b e encouraged, b e c a u s e a c o h e r e n t formalism (i.e., methods for sepa­ rating the s c a l e s of motion and expressing the conservation equations that would b e valid for the global o c e a n , the near-shore and sur­ face layer mixing) may b e just around the corner.

A consistent depth-integrated formalism for the coupling of surface waves and the m e a n flow is now well established. However, s o m e effects of surface mixing can only b e represented by vertically distributed equations of motion. The recent derivation by Mellor [2003] of three-dimensional equations for the current, with wave effects represented by "forcing terms" is a clear step toward a c o h e r e n t description of o c e a n dynamics that needs to b e verified, with wave forcing translated into ready-to-use forms.

Jenkins [1989] proposed to c o m p u t e

wave-forcing terms from the wave spectra computed by a wave model. Although the details of the parameterizations must b e worked out, this approach will benefit from the capability of wave models and their continual improvements. As comprehensive parameterizations of wave effects are developed from wave models, the wave models themselves will benefit from a careful c h e c k on the reliability of new para­ meters that will have to b e derived from the wave spectrum: Stokes drift, Stokes transport, m e a n surface slope, etc.

The d e m a n d for consistency between wave and m e a n flow dynamics and energetics is already promoting a re-examination of the basic physics of wave "dissipation" due to the formation of whitecaps (the most uncertain parameterized process in wave m o d e l s ) , and important insights will likely c o m e from prop­ erly understood radar measurements.

This joint use of wave and circulation models is an opportunity to bring the air-sea flux para­ meterizations used in atmosphere and o c e a n models in line with recent advances, in partic­ ular on the effect of wave age on the wind stress

[e.g.,Drennan et al, 2003] .This effect is probably

the largest and easiest improvement that c a n b e

m a d e in today's o c e a n or atmosphere circula­ tion models by using wave information. Great benefits were demonstrated for storm surge modeling [e.g.,Mastenbroek etai, 1993] and weather forecasting at the European Centre for Medium-Range Weather Forecasts (ECMWF)

[Janssen et al, 2 0 0 2 ] .

New observations have revealed strong effects of swells on the magnitude and direction of the wind stress [e.g., Grachev et al, 2 0 0 3 ] , and other studies suggest that the wind drag coef­ ficient may saturate at large wind speeds. These findings have important implications for climate models and hurricane forecasting, and have yet to b e translated into predictive parameterizations.

In summary, wave and circulation m o d e l s c a n already b e modified in the following ways to a c c o u n t for wave effects: modification of the wind drag coefficient ( d e p e n d e n c e on wave a g e ) ; use of surface currents for wave forecasting; inclusion of wave radiation stresses for the inner shelf/surf z o n e circulation; addi­ tion of a dynamically consistent formulation for Stokes drift for calculating near-surface drift velocities, in both deep and shallow water, and interpreting remotely sensed surface cur­ rents [e.g.,Broche et ai, 1983]; and use of the wave energy dissipation as an energy flux into the o c e a n to determine surface mixing bottom friction accounting for the roughness induced by the wave boundary layer roughness. Formal­ ism and parameterizations exist for all these effects, but only the first, s e c o n d , and third (for the surf z o n e only) have b e e n tested and vali­ dated in field conditions.

Thus, a wide research field is open.This research field also includes the following effects for which parameterizations, if they exist, are not well tested and observation and theory are s o m e t i m e s still shaky: modification of the wind drag coefficient by swell, sea state impact on air-sea heat fluxes, surface mixing due to Langmuir circulations ( L C s ) , a n d wave propagation over LCs.

However large the uncertainty on these latter effects, it is held that the first set of

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wave-Eos, Vol. 86, No.

4,

25 January 2005

dependent parameterization is enough to make the wave-circulation c o m b i n a t i o n useful, in particular when surface drift or sediment sus­ pension and transport is c o n s i d e r e d . T h e argu­ ment that o c e a n circulation models may not b e able to a c c o m m o d a t e the complexity and computer time required for a wave model does not stand, and many coupled numerical experiments have disproved it.

Operational Oceanography

The distribution of temperature and salinity beyond its impact on o c e a n biology, is all-important for the propagation of sound waves, and this has led to the establishment of opera­ tional circulation prediction models, essentially catering to naval needs.The n e e d s of the mili­ tary persist, but new applications are emerging.

Information d e m a n d e d by the public varies greatly with activities. Fishermen are interested in s e a state, to determine whether they c a n go out to fish, and in surface temperature to know where fish are to b e found. Surfers want to know the height and shape of breakers in particular spots.The offshore industry requires design criteria (wave plus current forces) for structures and routine forecasts of waves and currents for the operation of platforms.The shipping industry would like to gain time and m o n e y by optimizing routes, which requires wave forecasting and benefits from surface current forecasts. And, authorities n e e d to understand the transport and evolution of pollutants and nutrients. All of this information c a n b e provided by short-term forecasting sys­ tems fed by real-time data.

S o m e of this capability is being put in p l a c e in the framework of admirable collaborative efforts such as the Global O c e a n Observing System (GOOS) and its regional associated programs, side by side with o c e a n modeling efforts performed on a routine basis in civilian weather centers (such as forecasting waves, surface drift, and storm surges) or dedicated o c e a n o g r a p h i c centers.There is still an effort n e e d e d to make consistent use of these resources.

In coastal areas, waves have a large influence b e c a u s e their energy is not so much dwarfed by large-scale vorticity dynamics. Improving our understanding and capacity to forecast waves requires better coastal measurements; the dissemination of those measurements (many wave gauges around the world do not report data to the World Meteorological Orga­ nization); and a better description of the off­ shore wave field, including its directional properties, b e c a u s e waves generally c o m e from offshore. Observing systems should ben­ efit from a wider use of synthetic aperture radars (SARs), using the extended capabilities and wider swath coverage of recent instruments such as ENVISAT's ASAR. A great step forward c a n also b e m a d e with short-lived, low-cost satellite missions to measure wave spectra more directly and more accurately, such as the SWIMSAT mission being considered by the European S p a c e Agency

Increasing the a c c u r a c y of wave and circu­ lation models for those applications will nec­ essarily lead to more realistic parameterizations of unresolved processes. S o m e of this realism c a n b e obtained by coupling wave and circu­ lation models in a consistent way This task requires looking at the full complexity of the o c e a n , using well-tested parameterizations based on first principles for, e.g., drag coeffi­ cients, roughness lengths, and mixing coeffi­ cients.

A truly integrative effort with contributions from atmospheric s c i e n c e s and oceanography, including waves and remote sensing, is needed to put all current knowledge to work and thereby identify the weaknesses that will open the way to new research.

Further information c a n b e obtained from the Web site: http://surfouest.free.fr/WOO2003/.

References

Broche,P,J.C.de Maistre,and PForget (1983),Mesure par radar decametrique coherent des courants superficiels engendres par le vent, Oceanol.Acta, 6(1), 43-53.

Drennan,W M., H. C. Graber, D. Hauser, and C. Quentin (2003), On the wave age dependence of wind stress over pure wind seas,./ Geophys. Res., 108'(C3), 8062, doi:10.1029/2000JC000715.

Grachev, A. A., C. W Fairall, J. E. Hare, J. B. Edson, and S. D. Miller (2003), Wind stress vector over ocean waves. J. Phys. Oceanogr., 33,2408-2429. Hasselmann, K. (1991), Epilogue: waves, dreams, and

visions, in Directional ocean wave spectra, edited by R. Beal, pp. 205-208, Appl. Phys. Lab., Johns Hopkins Univ., Laurel, Md.

Janssen, PA. E.M.,J. D. Doyle, J. Bidlot, B. Hansen, L.Isaksen,and PViterbo (2002), Impact and feed­ back of ocean waves on the atmosphere, in

Advances in Fluid Mechanics, Atmos.-Ocean Inter­ actions Set, vol. I, edited by W Perrie, pp. 155-197,

MIT Press, Cambridge, Mass.

Jenkins, A. D. (1989),The use of a wave prediction model for driving a near-surface current model,

Dtsch. Hydrogr.Z.,42,133-149.

Mastenbroek, C, G. Burgers, and PA. E. M. Janssen (1993),The dynamical coupling of a wave model and a storm surge model through the atmospheric boundary layer. J. Phys. Oceanogr., 23,1856-1867. Mellor, G. (2003),The three-dimensional current and

surface wave equations. J. Phys. Oceanogr., 33, 1978-1989.

Mellor, G, and A. Blumberg (2004),Wave breaking and ocean surface layer thermal response, J. Phys.

Oceanogr, 34,693-698.

Reniers,A.J.H.M.,J.A. Roelvink and E. B.Thornton (2004) Morphodynamic modeling of an embayed beach under wave group forcing, J. Geophys. Res., 709,COlO3O,doi:lO.lO29/2OO2JCOO1586.

Santala,M. J., and E.A.Terray (1992) A technique for making unbiased estimates of current shear from a wave-follower,Deep Sea Res., 39,607-622.

Author Information

Fabrice Ardhuin, Centre Militaire d'Oceanographie, Service Hydrographique et Oceanographique de la Marine, Brest, France; Alastair D. Jenkins, Bjerkens Center for Climate Research, Geophysical Institute, University of Bergen, Norway; Daniele Hauser, Centre d'Etude des Environnements Terrestres et Planetaires,Velizy, France; Ad Reniers, Faculty of Civil Engineering and Geosciences, Delft University of Technology, Delft, Netherlands; and Bertrand Chapron, Laboratoire d'Oceanographie Spatiale, Ifre-mer, Plouzane, France

For additional information, contact FArdhuin; E-mail: Ardhuin@shom.fr.

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Page 37

Total wind stress xa

wind stress for waves (wind input): x m

wind stress for mean flow xa- xi n ,.

(direct) wave to mean flow stress (wave dissipation): x a i s

f (wave growth/decay )t

"normal" eddy diffusion

Mixing processes

Current boundary layer ( j f WavlfrJouMary IayeT" ^ |" ~ ' [

• * z = 0

Depth of penetration of the Stokes drift

mixed layer depth

Drift velocity profile U z ^ - <h> + 52 z = - </z> + 5 i — Z = - < / 7 > Sediments

fTg. /. Momentum fluxes and mixing processes coupling waves and currents. Processes for

horizontally uniform conditions, and possible profiles of eddy viscosity and drift velocity.

x{km)

5 7 9 11 13 15 0 1 2 3 4 5 -1.0 -0.6 -0.2 0.2 0.6 1.0 -2.0 -1.2 -0.4 0.4 1.2 2.0 Observed roughnness converted to wind speed (m/s) Hs (m) radial scatterer veiocities (mis) Radial tida! model velocity at 5 m depth frn/s)

Fig. 2. Illustration of sea-state impact on remote sensing. High-resolution information is extracted from a single synthetic aperture radar image acquired by ENVISAT over the coast of Normandy and the Channel Islands in March 2003. (Left) Surface roughness (radar cross section) interpreted in terms of wind speed but partly due to currents. (Middle left) Significant wave height computed from wave spectra. (Middle right) Radial velocity, positive to the west-southwest, due to surface drift, as seen by the radar. This surface drift is well correlated with the strong tidal currents (right panel shows modeled astronomical tidal currents) in that area and likely contains the Stokes drift due to waves. SAR data were provided by ESA, and image processing was performed by Fabrice Collard, Boost Technologies, Plouzane, France.

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