North Atlantic dynamical response to high latitude perturbations in buoyancy forcing Vassil Roussenov, Ric Williams & Chris Hughes How changes in the high.

Slides:



Advertisements
Similar presentations
Essentials of Oceanography
Advertisements

Wind-Driven Circulation in a Stratified Ocean Consider the ocean in several isopycnal layers that can be separated into two groups: Layers that outcrop.
Thermohaline circulation ●The concept of meridional overturning ●Deep water formation and property Antarctic Bottom Water North Atlantic Deep Water Antarctic.
Role of the Southern Ocean in controlling the Atlantic meridional overturning circulation Igor Kamenkovich RSMAS, University of Miami, Miami RSMAS, University.
Response of the Atmosphere to Climate Variability in the Tropical Atlantic By Alfredo Ruiz–Barradas 1, James A. Carton, and Sumant Nigam University of.
Propagation of wave signals along the western boundary and their link to ocean overturning in the North Atlantic Vassil Roussenov 1, Ric Williams 1 Chris.
Oceanic Circulation Current = a moving mass of water.
Background Tropopause theta composites Summary Development of TPVs is greatest in the Baffin Island vicinity in Canada, with development possibly having.
Baroclinic Instability in the Denmark Strait Overflow and how it applies the material learned in this GFD course Emily Harrison James Mueller December.
Propagation of wave signals in models and altimetry for the North Atlantic Vassil Roussenov 1, Chris Hughes 2, Ric Williams 1, David Marshall 3 and Mike.
The Ocean General Circulation (satellite)
Ocean Currents The Reality of Sending a Message in a Bottle.
Chapter 5: Other Major Current Systems
MODULATING FACTORS OF THE CLIMATOLOGICAL VARIABILITY OF THE MEXICAN PACIFIC; MODEL AND DATA. ABSTRACT. Sea Surface Temperature and wind from the Comprehensive.
Oceanic Circulation Current = a moving mass of water.
Mixing & Turbulence Mixing leads to a homogenization of water mass properties Mixing occurs on all scales in ocean –molecular scales (10’s of  m) –basin.
Lecture 7: The Oceans (1) EarthsClimate_Web_Chapter.pdfEarthsClimate_Web_Chapter.pdf, p
Wave communication of high latitude forcing perturbations over the North Atlantic Vassil Roussenov, Ric Williams & Chris Hughes How changes in the high.
Rapid Climate Change (RAPID) programme Meric Srokosz Southampton Oceanography Centre Natural Environment Research Council (NERC)
Topic 14 Density Driven Currents
Triggering of the Madden-Julian Oscillation by equatorial ocean dynamics. Benjamin G. M. Webber IAPSO-IAMAS JM10: Monsoons, Tropical Cyclones and Tropical.
Japan/East Sea Hybrid Coordinate Ocean Model (HYCOM) Patrick J. Hogan and Harley E. Hurlburt Naval Research Laboratory, Code 7323, Stennis Space Center,
The meridional coherence of the North Atlantic meridional overturning circulation Rory Bingham Proudman Oceanographic Laboratory Coauthors: Chris Hughes,
The meridional coherence of the North Atlantic meridional overturning circulation Rory Bingham Proudman Oceanographic Laboratory.
Two research cruises were successfully conducted in 2013 and Shipboard and moored observations show that: at first glance no significant decadal.
Model LSW formation rate (2 yr averages) estimated from: (red) CFC-12 inventories, (black) mixed layer depth and (green) volume transport residual. Also.
THE CONTRIBUTIONS OF CIMAS TO THE EVOLUTION OF PRESENT NOAA AND CLIVAR CLIMATE REQUIREMENTS.
Latitudinal Dependence of Atlantic Meridional Overturning Circulation (AMOC) Variations 2010 U.S. AMOC Annual Meeting June 7, 2010 Rong Zhang GFDL/NOAA.
General Ocean Circulation. Wind driven circulation About 10% of the water is moved by surface currents Surface currents are primarily driven by the wind.
Oceanic mesoscale variability and atmospheric convection on 10°N in the eastern Pacific Tom Farrar Thesis committee: Bob Weller, Raf Ferrari, Jim Price,
Transport in the Subpolar and Subtropical North Atlantic
Assuming 16 cm standard deviation. The final result – 5 of these records were noisy Halifax Grand Banks Line W 4100 m 2700 m 3250 m 2250 m 1800 m.
Ocean Circulation Currents. Horizontally Vertically.
Sara Vieira Committee members: Dr. Peter Webster
Ocean circulation Surface circulation driven by wind Subsurface circulation driven by density.
OCEAN CURRENTS.
Impact of partial steps and momentum advection schemes in a global ocean circulation model at eddy-premitting resolution Barnier Bernard et al.
Temporal Variability in the Physical Dynamics at Seamounts and its Consequence for Bio-Physical Interactions 2006 ROMS/TOMS European Workshop Universidad.
WOCE hydrographic Atlas, 1 As a result of the World Ocean Circulation Experiment (WOCE), a hydrographic survey of the world oceans occurred from
The Ocean General Circulation (satellite). Mean Circulation in the Ocean Gulf Stream.
The Southern Ocean geography, principal fronts, and oceanographic zones (see Table 13.1). The Subtropical Front (STF) is the oceanographic northern boundary.
Bifurcation Dynamics L. Gourdeau (1), B. Kessler (2) 1), LEGOS/IRD Nouméa, New Caledonia, 2) NOAA/PMEL, Seattle, USA Why is it important to study the bifurcation.
MOC related activities at NOC Joël Hirschi, Elaine McDonagh, Brian King, Gerard McCarthy Stuart Cunningham, Harry Bryden, Adam Blaker SAMOC workshop, Rio.
A Synthetic Drifter Analysis of Upper-Limb Meridional Overturning Circulation Interior Ocean Pathways in the Tropical/Subtropical Atlantic George Halliwell,
Cross-Gyre Thermohaline Transport in the Tropical Atlantic: The role of NBC Rings Bill Johns Zulema Garraffo Division of Meteorology and Physical Oceanography.
Mixing and Entrainment in the Orkney Passage Judy Twedt University of Washington Dept. of Physics NOAA, Geophysical Fluid Dynamics Lab Dr. Sonya Legg Dr.
Evaluation of two global HYCOM 1/12º hindcasts in the Mediterranean Sea Cedric Sommen 1, Alexandra Bozec 2, Eric P. Chassignet 2 Experiments Transport.
Waves in the coastal ocean - Coastal Oceanography - Aida Alvera-Azcárate
The relationship between sea level and bottom pressure in an eddy permitting ocean model Rory Bingham and Chris Hughes Proudman Oceanographic Laboratory.
IPCC AR4 Chapter 5 Oxygen decline at base of pycnocline throughout subpolar and subtropical N. Pacific: reduced ventilation Deutsch et al. (2005) IPCC.
Propagation of wave signals along the western boundary and their link to ocean overturning in the North Atlantic Vassil Roussenov 1, Ric Williams 1 Chris.
Forces and accelerations in a fluid: (a) acceleration, (b) advection, (c) pressure gradient force, (d) gravity, and (e) acceleration associated with viscosity.
Line W: A sustained measurement program sampling the North Atlantic Deep Western Boundary Current and Gulf Stream about 39°N 70°W Image copyrighted by.
Exploring the mesoscale activity in the Solomon Sea: a complementary approach with a numerical model and altimetric data L. Gourdeau 1, J. Verron 2, A.
Ocean Circulation. The Layered Ocean The oceans have a well-mixed surface layer of approximately 100 meters(300 feet) Layers of increasing density from.
ETESIAN WINDS AND COASTAL UPWELLING OVER THE NE AEGEAN SEA: MONITORING AND MODELING Yannis Androulidakis 1, Yannis Krestenitis 1, Villy Kourafalou 2 1.Laboratory.
Sea surface temperatures Sea water T varies with position in oceans Amount of insolation absorbed depends upon angle of incidence –With normal incidence,
Temperature and vertical stratification Metabolism: Q10 Preference & tolerance Poikilothermic or ectothermic vs. homeothermic or endothermic Thermocline.
Jake Langmead-Jones The Role of Ocean Circulation in Climate Simulations, Freshwater Hosing and Hysteresis Jake Langmead-Jones.
Chapter 3 Chemical and Physical Features of the Oceans Why study this?
(a) Sediments in the Ganges River plume in the northern Bay of Bengal
A Comparison of Profiling Float and XBT Representations of Upper Layer Temperature Structure of the Northwestern Subtropical North Atlantic Robert L.
Yongqiang Sun, Michael Ying, Shuguang Wang, Fuqing Zhang
Shelf-basin exchange in the Western Arctic Ocean
TAV / PIRATA-17 Meeting, Kiel, Germany
RAPID AND SLOW COMMUNICATION OF OVERTURNING
Linear and non-linear properties
What controls the time scale of Circumpolar Deep Water intrusions onto Antarctic continental shelves? Michael S. Dinniman Pierre St-Laurent John M. Klinck.
by M. A. Srokosz, and H. L. Bryden
Ocean Currents.
Presentation transcript:

North Atlantic dynamical response to high latitude perturbations in buoyancy forcing Vassil Roussenov, Ric Williams & Chris Hughes How changes in the high latitude thermohaline forcing communicate over the ocean? Downstream response at lower latitudes along the western boundary involving: fast, wave-like responses propagating against the sidewalls and along the equator an intermediate response involving changes in local circulation slower advective response Link with NERC RAPID monitoring programme, which aims to detect propagating wave signals along the western Atlantic from the bottom pressure and density signals. WAVE array (Western Atlantic Variability Experiment) is currently under way (Hughes, Marshall, Williams, Meredith & Foden). POL scientists (Hughes, Meredith, Foden, Pugh) + UKORS staff (Waddington) deployed bottom-pressure recorders and moorings along 2 sections in August 2004 and with WHOI deploying equipment in April 2004 (Toole, Hughes)

Surface layer thickness after an overturning of 10 Sv is switched on at time t = 0 on the northern boundary of the domain (Johnson and Marshall, 2002, JPO) Using an idealised model, Johnson and Marshall (2002) demonstrate how overturning changes are communicated through the propagation of fast Kelvin and slower Rossby waves. Background Kawase (1987) suggested, that the deep water spreading is accompanied by fast Kelvin waves, producing tropical sea surface temperature anomalies. Is there any evidence of a similar response in more complex models or in the observations?

Model set-up Model simulations carried out using an isopycnic model (MICOM). Horisontal resolution is 0.28º (30 km at the equator & 15km at 60N), 6 isopycnal layers. Model initialised from Levitus and forced by annual winds for 44 years. Thermohaline forcing is simulated by relaxation of model isopycnals to Levitus within the northern part of the basin. Initial adjustment twin experiment. Twin perturbation experiments during the last 4 years, where interfaces raised 120m/10 days over northern relaxation zone. Model tracer released in the relaxation zone. Model topography (ETOPO5)

Initial adjustment movie Model SSH (left) and deep interface pressure (right) anomalies (reference – disturbed fields). No wind forcing; adjustment to the initial vertical stratification. 2 model years movie, year 2-3.

Twin experiment movie Model SSH and bottom pressure anomalies (reference – disturbed fields) from the twin experiment forced by annual mean wind forcing. 4 model years movie, year

Snapshots Model snapshots of the sea surface height anomaly and the depth/pressure of a dense isopycnal there is a rapid spreading along the western boundary a slower spreading along the eastern boundary the SSH and isopycnal height anomalies appear related, but with SSH signals on a slightly broader scale. slow advective response, marked by the Labrador tracer day 5 Year 4 tracer Year 1 Year 2 Year 3 Year 4

Twin experiment time series green is default, black is perturbed model run, red is Labrador Sea tracer. fast wave response; range of frequencies; wave interactions, modulation Kelvin waves, coastal Rossby, hybrid? Interactions between waves and the circulation an intermediate response involving changes in local circulation slower deep advection Propagation of signals along the western boundary Hovmueler diagram along the western boundary from years (tracer in contours)

Correlation patterns Correlation of high pass filtered altimetry everywhere with that averaged in the northern NE Atlantic (100 grid point section marked in black dots). Places where correlation is not significant at the 95% level are left white (Hughes & Meredith), Signals correlate on western N. Atlantic and eastern edge of the N. Atlantic With no wind forcing, there is band of positive correlation all around the edge of the basin. With wind forcing, the correlation pattern is similar, but with an opposite sign on each side of the basin. Thus, the propagation of the anomalies has altered. Model results show a broadly similar character to the analytical and altimetric diagnostics. Role of background flow needs to be explored. Model correlation patterns for SSH without and with a background circulation (left panel, after 1 y of model run with no forcing; right panel, after 44 y of model run with wind forcing). +

Conclusions How changes in the high latitude thermohaline forcing communicate over the ocean? Downstream response at lower latitudes along the western boundary involving: fast wave responses propagating against the sidewalls and along the equator an intermediate response involving changes in local circulation slower advective response higher horisontal and vertical model resolution precise diagnostics to identify different responses, type of the waves, physical mechanisms semi-idealised experiments – real topography, simplified forcing real forcing simulations in order to link with and support the RAPID monitoring programme Future work The monitoring aims to detect propagating wave signals along the western Atlantic from the bottom pressure and density signals. Thus, the programme aims to understand how overturning signals are communicated. Map of deployment along 3 sections (thick line in left panel) and mooring schematic (right panel).