The Mid-Ocean Dynamics Experiment
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Role of Regional Ocean Dynamics in Dynamic Sea Level Projections by the End of the 21St Century Over Southeast Asia
EGU21-8618, updated on 25 Sep 2021 https://doi.org/10.5194/egusphere-egu21-8618 EGU General Assembly 2021 © Author(s) 2021. This work is distributed under the Creative Commons Attribution 4.0 License. Role of Regional Ocean Dynamics in Dynamic Sea Level Projections by the end of the 21st Century over Southeast Asia Dhrubajyoti Samanta1, Svetlana Jevrejeva2, Hindumathi K. Palanisamy2, Kristopher B. Karnauskas3, Nathalie F. Goodkin1,4, and Benjamin P. Horton1 1Nanyang Technological University, Singapore ([email protected]) 2Centre for Climate Research Singapore, Singapore 3University of Colorado Boulder, USA 4American Museum of Natural History, USA Southeast Asia is especially vulnerable to the impacts of sea-level rise due to the presence of many low-lying small islands and highly populated coastal cities. However, our current understanding of sea-level projections and changes in upper-ocean dynamics over this region currently rely on relatively coarse resolution (~100 km) global climate model (GCM) simulations and is therefore limited over the coastal regions. Here using GCM simulations from the High-Resolution Model Intercomparison Project (HighResMIP) of the Coupled Model Intercomparison Project Phase 6 (CMIP6) to (1) examine the improvement of mean-state biases in the tropical Pacific and dynamic sea-level (DSL) over Southeast Asia; (2) generate projection on DSL over Southeast Asia under shared socioeconomic pathways phase-5 (SSP5-585); and (3) diagnose the role of changes in regional ocean dynamics under SSP5-585. We select HighResMIP models that included a historical period and shared socioeconomic pathways (SSP) 5-8.5 future scenario for the same ensemble and estimate the projected changes relative to the 1993-2014 period. -
Significant Dissipation of Tidal Energy in the Deep Ocean Inferred from Satellite Altimeter Data
letters to nature 3. Rein, M. Phenomena of liquid drop impact on solid and liquid surfaces. Fluid Dynamics Res. 12, 61± water is created at high latitudes12. It has thus been suggested that 93 (1993). much of the mixing required to maintain the abyssal strati®cation, 4. Fukai, J. et al. Wetting effects on the spreading of a liquid droplet colliding with a ¯at surface: experiment and modeling. Phys. Fluids 7, 236±247 (1995). and hence the large-scale meridional overturning, occurs at 5. Bennett, T. & Poulikakos, D. Splat±quench solidi®cation: estimating the maximum spreading of a localized `hotspots' near areas of rough topography4,16,17. Numerical droplet impacting a solid surface. J. Mater. Sci. 28, 963±970 (1993). modelling studies further suggest that the ocean circulation is 6. Scheller, B. L. & Bous®eld, D. W. Newtonian drop impact with a solid surface. Am. Inst. Chem. Eng. J. 18 41, 1357±1367 (1995). sensitive to the spatial distribution of vertical mixing . Thus, 7. Mao, T., Kuhn, D. & Tran, H. Spread and rebound of liquid droplets upon impact on ¯at surfaces. Am. clarifying the physical mechanisms responsible for this mixing is Inst. Chem. Eng. J. 43, 2169±2179, (1997). important, both for numerical ocean modelling and for general 8. de Gennes, P. G. Wetting: statics and dynamics. Rev. Mod. Phys. 57, 827±863 (1985). understanding of how the ocean works. One signi®cant energy 9. Hayes, R. A. & Ralston, J. Forced liquid movement on low energy surfaces. J. Colloid Interface Sci. 159, 429±438 (1993). source for mixing may be barotropic tidal currents. -
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Vol. 62 Bollettino Vol. 62 - SUPPLEMENT 1 pp. 327 di Geofisica An International teorica ed applicata Journal of Earth Sciences IMDIS 2021 International Conference on Marine Data and Information Systems 12-14 April, 2021 Online Book of Abstracts SUPPLEMENT 1 Guest Editors: Michèle Fichaut, Vanessa Tosello, Alessandra Giorgetti BOLLETTINO DI GEOFISICA teorica ed applicata 210109 - OGS.Supp.Vol62.cover_08dorso19.indd 3 03/05/21 10:54 EDITOR-IN-CHIEF D. Slejko; Trieste, Italy EDITORIAL COUNCIL SUBSCRIPTIONS 2021 A. Camerlenghi, N. Casagli, F. Coren, P. Del Negro, F. Ferraccioli, S. Parolai, G. Rossi, C. Solidoro; Trieste, Italy ASSOCIATE EDITORS A. SOLID EaRTH GeOPHYsICs N. Abu-Zeid; Ferrara, Italy J. Ba; Nanjing, China R. Barzaghi; Milano, Italy J. Boaga; Padova, Italy C. Braitenberg; Trieste, Italy A. Casas; Barcelona, Spain G. Cassiani; Padova, Italy F. Cavallini; Trieste, Italy A. Del Ben; Trieste, Italy P. dell’Aversana; San Donato Milanese, Italy C. Doglioni; Roma, Italy F. Ferrucci, Vibo Valentia, Italy E. Forte; Trieste, Italy M.-J. Jimenez; Madrid, Spain C. Layland-Bachmann, Berkeley, U.S.A. Bollettino di Geofisica Teorica ed Applicata G. Li; Zhoushan, China c/o Istituto Nazionale di Oceanografia P. Paganini; Trieste, Italy e di Geofisica Sperimentale V. Paoletti, Naples, Italy Borgo Grotta Gigante, 42/c E. Papadimitriou; Thessaloniki, Greece 34010 Sgonico, Trieste, Italy R. Petrini; Pisa, Italy e-mail: [email protected] M. Pipan; Trieste, Italy G. Seriani; Trieste, Italy http-server: bgta.eu A. Shogenova; Tallin, Estonia E. Stucchi; Milano, Italy S. Trevisani; Venezia, Italy M. Vellico; Trieste, Italy A. Vesnaver; Trieste, Italy V. Volpi; Trieste, Italy A. -
Sustained Global Ocean Observing Systems
Introduction Goal The ocean, which covers 71 percent of the Earth’s surface, The goal of the Climate Observation Division’s Ocean Climate exerts profound influence on the Earth’s climate system by Observation Program2 is to build and sustain the in situ moderating and modulating climate variability and altering ocean component of a global climate observing system that the rate of long-term climate change. The ocean’s enormous will respond to the long-term observational requirements of heat capacity and volume provide the potential to store 1,000 operational forecast centers, international research programs, times more heat than the atmosphere. The ocean also serves and major scientific assessments. The Division works toward as a large reservoir for carbon dioxide, currently storing 50 achieving this goal by providing funding to implementing times more carbon than the atmosphere. Eighty-five percent institutions across the nation, promoting cooperation of the rain and snow that water the Earth comes directly from with partner institutions in other countries, continuously the ocean, while prolonged drought is influenced by global monitoring the status and effectiveness of the observing patterns of ocean temperatures. Coupled ocean-atmosphere system, and providing overall programmatic oversight for interactions such as the El Niño-Southern Oscillation (ENSO) system development and sustained operations. influence weather and storm patterns around the globe. Sea level rise and coastal inundation are among the Importance of Ocean Observations most significant impacts of climate change, and abrupt Ocean observations are critical to climate and weather climate change may occur as a consequence of altered applications of societal value, including forecasts of droughts, ocean circulation. -
Chapter 2: Ocean Observations
Chapter 2. Ocean observations 2.1 Observational methods With the rapid advancement in technology, the instruments and methods for measuring oceanic circulation and properties have been quickly evolving. Nevertheless, it is useful to understand what types of instruments have been available at different points in oceanographic development and their resolution, precision, and accuracy. The majority of oceanographic measurements so far have been made from research vessels, with auxiliary measurements from merchant ships and coastal stations. Fig. 2.1 Research vessel. Accuracy: The difference between a result obtained and the true value. Precision: Ability to measure consistently within a given data set (variance in the measurement itself due to instrument noise). Generally the precision of oceanographic measurements is better than the accuracy. 2.1.1 Measurements of depth. Each oceanographic variable, such as temperature (T), salinity (S), density , and current , is a function of space and time, and therefore a function of depth. In order to determine to which depth an instrument has been deployed, we need to measure ``depth''. Depth measurements are often made with the measurements of other properties, such as temperature, salinity and current. Meter wheel. The wire is passed over a meter wheel, which is simply a pulley of known circumference with a counter attached to the pulley to count the number of turns, thus giving the depth the instrument is lowered. This method is accurate when the sea is calm with negligible currents. In reality, research vessels are moving and currents might be strong, and thus the wire is not straight. The real depth is shorter than the distance the wire paid out. -
Shallow Water Waves and Solitary Waves Article Outline Glossary
Shallow Water Waves and Solitary Waves Willy Hereman Department of Mathematical and Computer Sciences, Colorado School of Mines, Golden, Colorado, USA Article Outline Glossary I. Definition of the Subject II. Introduction{Historical Perspective III. Completely Integrable Shallow Water Wave Equations IV. Shallow Water Wave Equations of Geophysical Fluid Dynamics V. Computation of Solitary Wave Solutions VI. Water Wave Experiments and Observations VII. Future Directions VIII. Bibliography Glossary Deep water A surface wave is said to be in deep water if its wavelength is much shorter than the local water depth. Internal wave A internal wave travels within the interior of a fluid. The maximum velocity and maximum amplitude occur within the fluid or at an internal boundary (interface). Internal waves depend on the density-stratification of the fluid. Shallow water A surface wave is said to be in shallow water if its wavelength is much larger than the local water depth. Shallow water waves Shallow water waves correspond to the flow at the free surface of a body of shallow water under the force of gravity, or to the flow below a horizontal pressure surface in a fluid. Shallow water wave equations Shallow water wave equations are a set of partial differential equations that describe shallow water waves. 1 Solitary wave A solitary wave is a localized gravity wave that maintains its coherence and, hence, its visi- bility through properties of nonlinear hydrodynamics. Solitary waves have finite amplitude and propagate with constant speed and constant shape. Soliton Solitons are solitary waves that have an elastic scattering property: they retain their shape and speed after colliding with each other. -
An Unconditionally Stable Scheme for the Shallow Water Equations*
810 MONTHLY WEATHER REVIEW VOLUME 128 An Unconditionally Stable Scheme for the Shallow Water Equations* MOSHE ISRAELI Computer Science Department, Technion, Haifa, Israel NAOMI H. NAIK AND MARK A. CANE Lamont-Doherty Earth Observatory, Columbia University, Palisades, New York (Manuscript received 24 September 1998, in ®nal form 1 March 1999) ABSTRACT A ®nite-difference scheme for solving the linear shallow water equations in a bounded domain is described. Its time step is not restricted by a Courant±Friedrichs±Levy (CFL) condition. The scheme, known as Israeli± Naik±Cane (INC), is the offspring of semi-Lagrangian (SL) schemes and the Cane±Patton (CP) algorithm. In common with the latter it treats the shallow water equations implicitly in y and with attention to wave propagation in x. Unlike CP, it uses an SL-like approach to the zonal variations, which allows the scheme to apply to the full primitive equations. The great advantage, even in problems where quasigeostrophic dynamics are appropriate in the interior, is that the INC scheme accommodates complete boundary conditions. 1. Introduction is easy to code and boundary conditions for the discre- The two-dimensional linearized shallow water equa- tized equations are fairly natural to impose. At the other tions represent the evolution of small perturbations in end of the spectrum, the CP algorithm is speci®cally the ¯ow ®eld of a shallow basin on a rotating sphere. designed with the characteristics of the physics of the Our interest in these model equations arises from our equatorial ocean dynamics in mind. By separating the interest in solving for the motions in a linear beta-plane free modes into the eastward propagating Kelvin mode deep ocean. -
The Contribution of Wind-Generated Waves to Coastal Sea-Level Changes
1 Surveys in Geophysics Archimer November 2011, Volume 40, Issue 6, Pages 1563-1601 https://doi.org/10.1007/s10712-019-09557-5 https://archimer.ifremer.fr https://archimer.ifremer.fr/doc/00509/62046/ The Contribution of Wind-Generated Waves to Coastal Sea-Level Changes Dodet Guillaume 1, *, Melet Angélique 2, Ardhuin Fabrice 6, Bertin Xavier 3, Idier Déborah 4, Almar Rafael 5 1 UMR 6253 LOPSCNRS-Ifremer-IRD-Univiversity of Brest BrestPlouzané, France 2 Mercator OceanRamonville Saint Agne, France 3 UMR 7266 LIENSs, CNRS - La Rochelle UniversityLa Rochelle, France 4 BRGMOrléans Cédex, France 5 UMR 5566 LEGOSToulouse Cédex 9, France *Corresponding author : Guillaume Dodet, email address : [email protected] Abstract : Surface gravity waves generated by winds are ubiquitous on our oceans and play a primordial role in the dynamics of the ocean–land–atmosphere interfaces. In particular, wind-generated waves cause fluctuations of the sea level at the coast over timescales from a few seconds (individual wave runup) to a few hours (wave-induced setup). These wave-induced processes are of major importance for coastal management as they add up to tides and atmospheric surges during storm events and enhance coastal flooding and erosion. Changes in the atmospheric circulation associated with natural climate cycles or caused by increasing greenhouse gas emissions affect the wave conditions worldwide, which may drive significant changes in the wave-induced coastal hydrodynamics. Since sea-level rise represents a major challenge for sustainable coastal management, particularly in low-lying coastal areas and/or along densely urbanized coastlines, understanding the contribution of wind-generated waves to the long-term budget of coastal sea-level changes is therefore of major importance. -
Guidelines Towards an Integrated Ocean Observation System for Ecosystems and Biogeochemical Cycles
GUIDELINES TOWARDS AN INTEGRATED OCEAN OBSERVATION SYSTEM FOR ECOSYSTEMS AND BIOGEOCHEMICAL CYCLES Hervé Claustre(1), David Antoine(1), Lars Boehme(2), Emmanuel Boss(3), Fabrizio D’Ortenzio(1), Odile Fanton D’Andon(4), Christophe Guinet(5), Nicolas Gruber(6), Nils Olav Handegard(7), Maria Hood(8), Ken Johnson(9), Arne Körtzinger(10), Richard Lampitt(11), Pierre-Yves LeTraon(12), Corinne Lequéré(13), Marlon Lewis(14), Mary-Jane Perry(15), Trevor Platt(16), Dean Roemmich(17), Shubha Sathyendranath(16), Uwe Send(17), Pierre Testor(18), Jim Yoder(19) (1) CNRS and University P. & M. Curie, Laboratoire d’Océanographie de Villefranche, 06230 Villefranche-sur-mer, France, Email: [email protected], [email protected], [email protected] (2) NERC Sea Mammal Research Unit, Scottish Oceans Institute, University of St Andrews, St Andrews, Fife KY16 8LB, Scotland, UK, Email: [email protected] (3) University of Maine, School of Marine Science, Orono, ME 04469 USA, Email: [email protected] (4) ACRI-ST, 260, route du Pin Montard - B.P. 234, 06904 Sophia Antipolis Cedex, France, Email: [email protected] (5) CNRS, Centre d'Etudes Biologiques de Chizé, Villiers-en-Bois, 79360 Beauvoir-sur-niort , France, [email protected] (6) Institute of Biogeochemistry and Pollutant Dynamics, ETH Zurich, Universitatstrasse 16, 8092 Zurich, Switzerland, Email: [email protected] (7) Institute of Marine Research, Postboks 1870 Nordnes, 5817 Bergen, Norway, Email: [email protected] (8) UNESCO-IOC, 1 Rue Miollis, 75732 Paris cedex 15, France, Email: [email protected] (9) Monterey Bay Aquarium Research Institute 7700 Sandholdt Road Moss Landing, CA 95039, USA, Email: [email protected] (10) Leibniz-Institut für Meereswissenschaften (IFM-GEOMAR) Chemische Ozeanographie Düsternbrooker Weg 20, 24105 Kiel, Germany. -
Geophysical Fluid Dynamics, Nonautonomous Dynamical Systems, and the Climate Sciences
Geophysical Fluid Dynamics, Nonautonomous Dynamical Systems, and the Climate Sciences Michael Ghil and Eric Simonnet Abstract This contribution introduces the dynamics of shallow and rotating flows that characterizes large-scale motions of the atmosphere and oceans. It then focuses on an important aspect of climate dynamics on interannual and interdecadal scales, namely the wind-driven ocean circulation. Studying the variability of this circulation and slow changes therein is treated as an application of the theory of nonautonomous dynamical systems. The contribution concludes by discussing the relevance of these mathematical concepts and methods for the highly topical issues of climate change and climate sensitivity. Michael Ghil Ecole Normale Superieure´ and PSL Research University, Paris, FRANCE, and University of California, Los Angeles, USA, e-mail: [email protected] Eric Simonnet Institut de Physique de Nice, CNRS & Universite´ Coteˆ d’Azur, Nice Sophia-Antipolis, FRANCE, e-mail: [email protected] 1 Chapter 1 Effects of Rotation The first two chapters of this contribution are dedicated to an introductory review of the effects of rotation and shallowness om large-scale planetary flows. The theory of such flows is commonly designated as geophysical fluid dynamics (GFD), and it applies to both atmospheric and oceanic flows, on Earth as well as on other planets. GFD is now covered, at various levels and to various extents, by several books [36, 60, 72, 107, 120, 134, 164]. The virtue, if any, of this presentation is its brevity and, hopefully, clarity. It fol- lows most closely, and updates, Chapters 1 and 2 in [60]. The intended audience in- cludes the increasing number of mathematicians, physicists and statisticians that are becoming interested in the climate sciences, as well as climate scientists from less traditional areas — such as ecology, glaciology, hydrology, and remote sensing — who wish to acquaint themselves with the large-scale dynamics of the atmosphere and oceans. -
Sea Level Rise Workshop Rpt.Pdf
SUMMARY REPORT FROM THE WORLD CLIMATE RESEARCH ROGRAMME WORKSHOP UNDERSTANDING SEA-LEVEL RISE AND VARIABILITY (Paris, France, 6-9 June 2006) SEPTEMBER 2006 WCRP Informal Report N° 20/2006 THE WORKSHOP. 163 scientists from 29 countries attended the Workshop on Understanding Sea-level 1 Rise and Variability, hosted by the Intergovernmental Oceanographic Commission of UNESCO in Paris Understanding Sea-level Rise and Variability World Climate Research Programme Workshop Summary Statement from the June 6-9, 2006. The Workshop was organized by the World Climate Research Programme (WCRP)2 to bring together all relevant scientific expertise with a view towards identifying the uncertainties associated with past and future sea-level rise and variability, as well as the research and observational activities needed for narrowing these uncertainties. The Workshop was also conducted in support of the Global Earth Observation System of Systems (GEOSS) 10-Year Implementation Plan;3 as such, it helped develop international and interdisciplinary scientific consensus for those observational requirements needed to address sea-level rise and its variability. The Issue – Since the beginning of high-accuracy satellite altimetry in the early 1990s, global mean sea-level has been observed by both tide gauges and altimeters to be rising at a rate of just above 3 mm/year, compared to a rate of less than 2 mm/year from tide gauges over the previous century. The extent to which this increase reflects natural variability versus anthropogenic climate change is unknown. About half of the sea-level rise during the first decade of the altimeter record can be attributed to thermal expansion due to a warming of the oceans; the other major contributions include the combined effects of melting glaciers and ice sheets. -
MAR 542 – Fundamentals of Atmosphere and Ocean Dynamics Instructor: Marat Khairoutdinov Room: 158 Endeavour Time: Tuesdays and Thursday 11:30 AM – 12:50 PM
MAR 542 – Fundamentals of Atmosphere and Ocean Dynamics Instructor: Marat Khairoutdinov Room: 158 Endeavour Time: Tuesdays and Thursday 11:30 AM – 12:50 PM Text: Atmosphere, Ocean, and Climate Dynamics: An Introductory Text By John R. Marshall and R. Alan Plumb, Academic Press 2008 This course serves as an introduction to atmosphere and ocean dynamics. It is required of first-year atmospheric science graduate students, and it is recommended for first-year physical oceanography students. It assumes a working knowledge of differential and integral calculus, including partial derivatives and simple differential equations. Its purpose is to prepare students in atmospheric sciences and physical oceanography to move onto more advanced courses in these areas, as well as to acquaint each other with some fundamental aspects of dynamics applied to geophysical fluids outside your area of specialization. It is anticipated that the entire book will be covered. The chapter contents of this text are as follows, but some other topics will also be covered. 1. Characteristics of the atmosphere 2. The global energy balance 3. The vertical structure of the atmosphere 4. Convection 5. The meridional structure of the atmosphere 6. The equations of fluid motion 7. Balanced flow 8. The general circulation of the atmosphere 9. The ocean and its circulation 10. The wind-driven circulation 11. The thermohaline circulation of the ocean 12. Climate and climate variability • !"#$"%"&'"()*"+(,&-.)*/*0-",+--"1-"2*3&4"5$"6,7" • 8+9:";&<*/-"+2&=(">$"%"&'"()*"?+/()0-"-=/'+;*7" • @)*"+<*/+A*":*.()"&'"()*"&;*+9-"1-"+2&=("B"6,7" • !C$"%"&'"()*"?+/()0-"3+9:"1-"19"()*"D&/()*/9"E*,1-.)*/*7" Atmosphere is very thin: 99.9% of mass is below 50 km Compared to the Earth’s radius (6500 km), it is only 1% which is comparable to the thickness of an apple’s skin Thus, the synoptic-scale systems are quasi-two-dimensional! Vertical structure of the atmosphere Pressure (mb) 0.001 0.01 0.1 1 10 100 1000 Permanent vs.