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High Baroclinic Equatorial Kelvin Waves and Central Pacific Surface Warming Peter C Chu Naval Postgraduate School Monterey, CA, USA Jilin Sun and Qinyu Liu Ocean University of China Qingdao, China Email: [email protected] http://www.oc.nps.navy.mil/~chu

High Baroclinic Equatorial Kelvin Waves and Central

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Page 1: High Baroclinic Equatorial Kelvin Waves and Central

High Baroclinic Equatorial Kelvin Waves and Central Pacific Surface

Warming

Peter C ChuNaval Postgraduate School Monterey, CA, USA

Jilin Sun and Qinyu LiuOcean University of China

Qingdao, ChinaEmail: [email protected]

http://www.oc.nps.navy.mil/~chu

Page 2: High Baroclinic Equatorial Kelvin Waves and Central

Outline

• Enhancing Counter Mode (ECM)

• Second Baroclinic Equatorial Kelvin Waves

• Two-Stage Air-Sea Interaction for the El Nino Onset

Page 3: High Baroclinic Equatorial Kelvin Waves and Central

Central Pacific Warming Prior to the El Nino Onsets in 90’s

Page 4: High Baroclinic Equatorial Kelvin Waves and Central

1997 El Nino – Central Pacific Warming (Picautet al. 2002)

Page 5: High Baroclinic Equatorial Kelvin Waves and Central

1997 El Nino – Westerly Wind Burst (Picaut et al. 2002)

Page 6: High Baroclinic Equatorial Kelvin Waves and Central

Equatorial Current System

Upper Layer: Westward FlowingSouth Equatorial Current (SEC)

Thermocline:Eastward FlowingEquatorial Counter Current (EUC)

Page 7: High Baroclinic Equatorial Kelvin Waves and Central

McPhaden et al. (JGR, 1998)

Page 8: High Baroclinic Equatorial Kelvin Waves and Central

Mean Current System

• Upper Layer– SEC (Westward)

• Thermocline – EUC (Eastward)

• Mean Surface Cold Advection (Mean Surface Temperature Decreasing Eastward)

Page 9: High Baroclinic Equatorial Kelvin Waves and Central

Perturbation Current System Enhancing Counter Mode

(ECM)

• Upper Layer Eastward Flow

• Thermocline westward Flow

• Reduction of Mean Surface Cold Advection

Page 10: High Baroclinic Equatorial Kelvin Waves and Central

Enhancing CM Detected from TAO Data

Page 11: High Baroclinic Equatorial Kelvin Waves and Central

Upper Layer and Thermocline (Wyrtki and Kilonsky 1984)

• Hawaii to Tahiti Temperature Data (1978-1980)

• Upper Layer

– Surface to 25oC depth

• Thermocline

– 25oC depth to 15oC depth

Page 12: High Baroclinic Equatorial Kelvin Waves and Central

(a) 165oE

(b) 140oW

Daily Mean Depths of 25oC (Solid) and 15oC (dashed) Isotherms at (a) 165oE, and (b) 140oW along the Equator.

Page 13: High Baroclinic Equatorial Kelvin Waves and Central

Enhancing CM detected from the TAO data at 165oE. Here solid (dashed) curve is the upper layer (thermocline) zonal speed anomaly.

Page 14: High Baroclinic Equatorial Kelvin Waves and Central

Time evolution of SST anomaly at 165oE (solid). Note that SST warm anomaly appears during the ECM periods.

Page 15: High Baroclinic Equatorial Kelvin Waves and Central

Time evolution of zonal wind speed anomaly (m/s) at 165oE obtained from the TAO data. Note that the west wind anomaly ( > 0) appears during the ECM periods.

Page 16: High Baroclinic Equatorial Kelvin Waves and Central

Simple Ocean Data Assimilation (SODA) System (Carton et al., 2000)

• MOM (NOAA/GFDL)

• 62oS – 62oN

• Data Assimilated– WOA-94– Satellite Altimetry (GEOSAT, ERS-1, T/P)

• Resolution: – Zonal 1o

– Meridional Varying, 0.4286o near the equator

Page 17: High Baroclinic Equatorial Kelvin Waves and Central

ECM Detected from SODA Data

• Monthly mean temperature and velocity data since 1950.

• SST

• Upper Layer Zonal Velocity

• Thermocline Zonal Velocity

Page 18: High Baroclinic Equatorial Kelvin Waves and Central

↓ ↓↓ ↓ ↓

↓↓

Upper Layer u’ (cm/s, Blue)Thermocline u’ (cm/s, Black)SST’ (oC * 12)at 165oE

Page 19: High Baroclinic Equatorial Kelvin Waves and Central

Upper Layer u’ (cm/s, Blue)Thermocline u’ (cm/s, Black)

SST’ (oC * 12)at 165oE

↓ ↓ ↓↓

Page 20: High Baroclinic Equatorial Kelvin Waves and Central

↓↓↓

Upper Layer u’ (cm/s, Blue)Thermocline u’ (cm/s, Black)SST’ (oC * 12)at 165oE

Page 21: High Baroclinic Equatorial Kelvin Waves and Central

↓ ↓

Upper Layer u’ (cm/s, Blue)Thermocline u’ (cm/s, Black)SST’ (oC * 12)at 165oE

Page 22: High Baroclinic Equatorial Kelvin Waves and Central

Upper Layer u’ (cm/s, Blue)Thermocline u’ (cm/s, Black)

SST’ (oC * 12)at 165oE

↓↓

Page 23: High Baroclinic Equatorial Kelvin Waves and Central

Upper Layer u’ (cm/s, Blue)Thermocline u’ (cm/s, Black)

SST’ (oC * 12)at 165oE

↓↓ ↓

Page 24: High Baroclinic Equatorial Kelvin Waves and Central

Propagation of Second-Baroclinic Kelvin Waves and ECM

Typical temperature profile and Brunt-Vaisala Frequency at the Equatorial Pacific

Page 25: High Baroclinic Equatorial Kelvin Waves and Central

Three gravest vertical modes for u’ calculated using a linear, continuously stratified, hydrostatic model with the Boussinesq approximation [after Philander, 1990]. Note that the node for the first baroclinic mode is at around 1500 m depth.

Page 26: High Baroclinic Equatorial Kelvin Waves and Central

Equatorial Layered Model (McCreary and Yu, 1992)

• 2 ½ (or 1 ½) - Layer – The First Two Layers Active– The Third Layer Motionless

• Momentum Balance• Heat Balance• Entrainment/Detrainment Rate• Wind Forcing • 1o X 1o Resolution

Page 27: High Baroclinic Equatorial Kelvin Waves and Central
Page 28: High Baroclinic Equatorial Kelvin Waves and Central

Model Parameters (McCreary and Yu, 1992)

Page 29: High Baroclinic Equatorial Kelvin Waves and Central

Model Area

15oN

15oS0o 100o

Page 30: High Baroclinic Equatorial Kelvin Waves and Central

Surface Winds (Trade Winds)

Y(y)=1 (No Latitudinal Variance).

T(t) = Ramp function that increases linearly from 0 to 1 in the first 5 days

Page 31: High Baroclinic Equatorial Kelvin Waves and Central

Zonal Variation of the Trade Winds

Page 32: High Baroclinic Equatorial Kelvin Waves and Central

Initial Conditions

Page 33: High Baroclinic Equatorial Kelvin Waves and Central

Model Integration

• (1) Model is integrated for 1080 days to reach nearly equilibrium state.

• (2) Westerly wind patch is added at day-1080 for 25 days, and then is removed.

• (3) Model is integrated for 1000 days.

Page 34: High Baroclinic Equatorial Kelvin Waves and Central

Control RunLayer Thickness Anomaly (m) at Day-1080:(a) 1st Layer, (b) 2nd Layer.

Page 35: High Baroclinic Equatorial Kelvin Waves and Central

Control RunHorizontal Currents at Day-1080.

(a) 1st Layer: SEC; 2nd Layer: EUC

Page 36: High Baroclinic Equatorial Kelvin Waves and Central

Westward Shift of the Trade Wind MaximumX = 53o

Westward Shift of Maximum Currents

Page 37: High Baroclinic Equatorial Kelvin Waves and Central

Trade Winds Reduced to 85%(a) SEC weakens

(b) EUC weakens

Page 38: High Baroclinic Equatorial Kelvin Waves and Central

Trade Winds Reduced to 70%

(a) SEC weakens

(b) EUC weakens

Page 39: High Baroclinic Equatorial Kelvin Waves and Central

Westerly Wind Burst Patch

Westerly wind = 10 m/s

Westerly wind patch is added at day-1080 for 25 days, and then is removed.

Page 40: High Baroclinic Equatorial Kelvin Waves and Central

Time-Longitude Cross Section of Zonal Velocity Anomaly (cm/s) : (a) 1st Layer, (b) 2nd Layer (Control Run)

Page 41: High Baroclinic Equatorial Kelvin Waves and Central

Time-Longitude Cross Section of Temperature Anomaly (oC) : (a) 1st Layer, (b) 2nd Layer (Control Run)

Page 42: High Baroclinic Equatorial Kelvin Waves and Central

Time-Longitude Cross Section of Zonal Velocity Anomaly (cm/s) : (a) 1st Layer, (b) 2nd Layer (Trade Wind Maximum Shifted Westward)

Page 43: High Baroclinic Equatorial Kelvin Waves and Central

Time-Longitude Cross Section of Temperature Anomaly (oC) : (a) 1st Layer, (b) 2nd Layer (Trade Wind Maximum Shifted Westward)

Page 44: High Baroclinic Equatorial Kelvin Waves and Central

Time-Longitude Cross Section of Zonal Velocity Anomaly (cm/s) : (a) 1st Layer, (b) 2nd Layer(Trade Winds Reduced to 85%)

Page 45: High Baroclinic Equatorial Kelvin Waves and Central

Time-Longitude Cross Section of Temperature Anomaly (oC) : (a) 1st Layer, (b) 2nd Layer (Trade Winds Reduced to 85% )

Page 46: High Baroclinic Equatorial Kelvin Waves and Central

Time-Longitude Cross Section of Zonal Velocity Anomaly (cm/s) : (a) 1st Layer, (b) 2nd Layer (Trade Winds Reduced to 70%)

Page 47: High Baroclinic Equatorial Kelvin Waves and Central

Time-Longitude Cross Section of Temperature Anomaly (oC) : (a) 1st Layer, (b) 2nd Layer (Trade Winds Reduced to 70% )

Page 48: High Baroclinic Equatorial Kelvin Waves and Central

Conclusions

• ECM weakens the surface cold advection that may lead to central Pacific warming

• Second baroclinic Kelvin waves cause ECM.

• Two-stage air-sea interaction mechanism is proposed for the El Nino onset.

Page 49: High Baroclinic Equatorial Kelvin Waves and Central

Two-Stage Air-Sea Interaction Mechanism