Lecture 13 El Niño/La Niña Ocean-Atmosphere Interaction. Idealized 3-Cell Model of Wind Patterns on a Rotating Earth. Previous Lecture!

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Lecture 13 El Niño/La Niña Ocean-Atmosphere Interaction Previous Lecture! Global Winds General Circulation of winds at the surface and aloft Polar Jet Stream Subtropical Jet Stream Monsoons 1 2 Radiation Budget at the top of the Earth s Atmosphere Idealized 3-Cell Model of Wind Patterns on a Rotating Earth A schematic of the Earth s weather machine bringing warm moist air northward and cold dry air southward (latent and sensible heat). Polar Cell Ferrel Cell Hadley Cell Hadley Cell Red Line is incoming radiation from the sun Blue Line is outgoing radiation emitted by the earth Ferrel Cell 3 4

Hadley Circulation in Action Equator to Pole Cross Section 5 6 Jet Streams Jet Stream has Waves Fast air currents, 1000 s of km s long, a few hundred km wide, a few km thick Differential heating causes polar jet Conservation of angular momentum explains subtropical jet 7 8

Waves in Jet Stream cause Storms El Niño La Niña Ocean-Atmosphere Interaction Wind speeds at 300mb (kt) (March 9 2005) Cloud cover Outline Ocean Circulation El Niño La Niña Southern Oscillation ENSO 9 10 Intro to Ocean Circulation The Ocean Currents are Driven by Winds t Gulf Stream Layer-mean water flow is at right angles to wind (to right in NH) as a result of the Coriolis force on the current. 11 12

Formation of Ocean Gyres Force Balance in an Ocean Gyre Anticyclonic winds cause water to pile up. Cyclonic wind result in a trough. The thermocline is marked by strong vertical temperature change with cold water below. Piling up of water lowers the thermocline. geostrophic balance? The wind-driven North Atlantic ocean gyre has clockwise (anticyclonic) flow in NH and is in ~geostrophic balance. 13 14 General Circulation - July Average surface ocean currents 15 16

Long term mean current speed (shaded) Shallow and deep currents This is a long term mean and streamlines derived from satellite altimetry and near-surface drifters. Nikolai Maximenko, IPRC. Deep ocean currents also exist e.g. after dense water sinks at high latitudes (where the water is less salty and cold i.e. dense) it returns southwards at great depth as part of the Global conveyor Belt 17 18 Coriolis force and upwelling Prevailing along-shore winds drive currents away from shore, producing upwelling of colder water from below. Cold upwelling is prevalent along the West Coast of the US (e.g., California) and Europe (Portugal). The resulting cool near-shore ocean water helps produce the dry Mediterranean climate these areas are known for. Why? Cold water supports low humidity. Coastal upwelling brings cold water to the surface Winds and Ocean Currents Summary High pressure dominates the subtropical North Atlantic and North Pacific in summer. This leads to the formation of an ocean gyre and clockwise currents in the ocean basins, and warm ocean currents on the east side of continents and cold currents on the west side of continents. 19 20

Why do we care about El Niño- Southern Oscillation (ENSO)? Droughts Increased Wild Fires Water supply Extreme Precipitation Floods Erosion Disease Transportation Impacts food chain and economy Agricultural productivity Impacts of El Niño 21 22 Impacts of El Niño El Niño-Southern Oscillation (ENSO) An Example of Estimated Losses from 1982/83 El Nino Event $8.11 Billion Every few years El Niño, a sea-surface temperature (SST) warming over the central equatorial Pacific Ocean, persists and is widespread. Alters weather patterns globally. Large ecosystem impacts and economic losses. Long timescale of ENSO (months) yields improved seasonal prediction. Better insight into coupled behavior of ocean and atmosphere may lead to better overall understanding of climate and climate change. 23 24

What is El Niño? The name El Niño (referring to the Christ child) was originally given by Peruvian fisherman to a warm current that appeared every few years around Christmas. The term El Niño refers to a rapid, dramatic warming of the sea-surface temperatures (SSTs) in the eastern and central equatorial Pacific, beginning along the north-central coast of South America and extending westward, that results in large-scale changes in the winds and rainfall patterns. Southern Oscillation The Southern Oscillation was named by Sir Gilbert Walker in 1923, who noted that "when pressure is high in the Pacific Ocean it tends to be low in the Indian Ocean from Africa to Australia". Walker was Director of Observatories in India and was mostly concerned with variations in the Indian monsoon. His was the first recognition that changes across the tropical Pacific and beyond were not isolated phenomena but were connected as part of a larger oscillation in equatorial SST that we now refer to as El Niño and La Niña. 25 26 Ocean ENSO Indices Correlate ENSO The complete phenomenon is known as the El Niño Southern Oscillation, or ENSO. The warm El Niño phase typically lasts for 8-10 months or so. The entire ENSO cycle lasts usually about 3-7 years, and includes a cold phase, known as La Niña, that may be similarly strong. However, the ENSO cycle is not a regular oscillation like the change of seasons, but can be highly variable in strength and timing. Atmosphere Surface Pressure Difference 27 28

Physical Explanation for ENSO Trade winds promote cold water upwelling in eastern tropical Pacific as a result of Coriolis force on currents. Cool, deep water is nutrient rich and supports rich ecosystem (plankton, fish, birds, ) Weaker trades lead to weaker upwelling. Warm nutrientpoor tropical water replaces the cold, nutrient-rich water. called El Niño (the boy in reference to its occurrence near Christmas) SST Maps During NH Winter Along Equator Along Peru 29 30 El Niño SST Anomalies La Niña SST Anomalies During el niño weaker easterly winds over the equator result in less upwelling and warmer SST. During la niña stronger easterly winds over the equator result in more upwelling and colder SST. 31 32

ENSO Animation ENSO Pressure Anomalies H L L H Average Sea-Level Atmospheric Pressure Anomalies (mb) for January through March associated with El Niño (left) and La Niña (right). 33 34 El Niño s Influence on Hawaii Climate Dry in the El Niño Winter Time series of El Niño Index El Niño of the Century warm C cool Normalized Hawaii rainfall index Enhanced subsidence due to strong convection in the central and eastern equatorial Pacific El Niño: peaks in the northern hemisphere winter months (Dec., Jan. Feb.) 35 36

1997698 1998699 Sea$surface$temperature$and$surface$winds$during$November6April$of$1997698,$and$1998699. Precipitation (CMAP) and surface winds (ERS-2) during Nov.-April of 1997-98, and 1998-99. 37 38 Ocean-Atmosphere Anomalies SST anomaly (colors) and SSM/I wind stress anomalies (vectors) for August 1997. Picaut et al. (2002, JGR) Chlorophyll shows where nutrient upwelling is taking place in Dec. 1997 and Dec. 1998 TRMM Rainfall Anomalies Jan 1998 39 40

Interaction of thermocline depth, SST and winds Satellite altimeters observe heat redistribution in the ocean (thick warm water layer in red & white) Dec 1997 Temperature along Equator Dec 1998 Wind anomalies Temperature anomalies 41 42 1997-1998 Nov.-April El Niño weak winds El Niño of the Century SST Warmer Ocean El Niño (Warm Phase) 1998-1999 Nov.-April normal winds Less Rain More rain TRMM$Rainfall$Anomalies$$Jan$1998 Weaker tradewinds leads less upwelling Warmest SSTs, convection & rainfall shift to central Pacific Warmer SST s in eastern Pacific 43 44

La Niña (cold phase) ENSO Neutral (Average) Winds and surface water flow toward west, upwelling Warmest SSTs, convection & rainfall shift to Western Pacific Colder SST s in eastern Pacific Surface water flow from east toward west, upwelling Deep thermocline and warm water in western Pacific (associated deep convection & rainfall) Shallow thermocline and cool SST s in east Pacific 45 46