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Mechanisms controlling ENSO: A simple hybrid coupled model study. Cheng-Wei Chang 1 * and Jia-Yuh Yu 2 1. Institute of Geography, Chinese Culture University, Taipei, Taiwan, cwchang@atmos.pccu.edu.tw , +886-2-28610511 ext25705
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Mechanisms controlling ENSO: A simple hybrid coupled model study Cheng-Wei Chang1* and Jia-Yuh Yu2 1. Institute of Geography, Chinese Culture University, Taipei, Taiwan, cwchang@atmos.pccu.edu.tw, +886-2-28610511 ext25705 2. Department of Atmospheric Sciences, Chinese Culture University
Contents • 1. Introduction • 2. Data Sources • 3. Mechanisms: 3-1、Westerly Wind Bursts 3-2、Non-homogeneous Air-sea Feedback • 4.Concluding Remarks
Introduction • During the cold epoch (1960s and 1970s), the ENSO scenario (viewed as SSTA) starts in the east and propagates westward along the equator. • During the warm epoch (1980s and 1990s), eastward propagating SSTA associated with westerly wind burst in the central Pacific strengthen ENSO ( Rasmusson and Carpenter 1982; Zhang and Busalacchi 1999).
The surface winds over the tropical Pacific Ocean show energetic large-scale variability on timescales ranging from a few days to decades (Luther et al. 1983; Luther and Harrison 1984; Harrison and Luther 1990). • The instability involves feedbacks between SST, which affects the atmospheric circulation, and the dynamics of the ocean circulation must adjust to the changes in wind.
Air-sea interaction over deep convection region The vertically-integrated moist static energy Quasi-equilibrium convective constraints assumption (Betts and Miller, 1986)(Yu and Neelin,1997)
Over deep convection region Long time average Gross moist stability (M) (Yu and Neelin,1997)
Data Sources • NCEP/NCAR re-analysis grid data of atmosphere • Reconstruction OI SST • Domain:90°N~90°S/0°E~0°W • Horizontal resolution: 2.5°×2.5° • Study period: 1949~2000
Simple Hybrid Coupled Model • Ocean Component – Cane-Zebiak (CZ) model with Niller-Kraus vertical mixing scheme • Atmospheric Component – Empirical atmospheric model based on SVD projections of the first 7 modes • Domain: 0°E~0°W/30°N~30°S • Horizontal resolution: 2°×1°
The OBS. westerly wind bursts • Hartten(1996) 1000-hPa zonal winds anomaly exceeded 5 m/s with a zonal extent over 10° and lasting 10days
Hybrid coupled model Feb. ½~Apr. ½ westerly wind bursts(Max 10m/s) 15°N 120°E 180°E 15°S
WWB effect Belamarl,2003 Feb. ½~Apr. ½ WWB can excite the ENSO-like pattern
The hybrid couple model simulates ENSO Feb. ½~Apr. ½ • Ideal exp. +WWB
Stand run Stand run+ WWB Feb. ½~Apr. ½ • What cause WWB? • how to maintain it in long time?
Gross moist stability (M) • climatology
Hybrid coupled model non-homogeneous air-sea feedback 15°N 120°E 180°E 15°S
Stand run Stand run+ WWB Stand run+ non-hom non-homogeneous air-sea feedback
Air-sea interaction increases interannual period 1.5years 1years 1.5years ~1years
Stand run Stand run+ non-hom Half period ~1 year Half period ~1.5 years It makes the WWBs effectively self-sustained in the tropical region
The decadal change of WWB • WWB’ strength and period in warm epoch are stronger and longer than in cold epoch
The decadal change of M • climatology • warm epoch
Stand run Stand run+warm Stand run+non-hom Decadal effect