On the Formation and Maintenance of the Interannual Variability of the North Atlantic Oscillation

Author:

Yang Yang12ORCID,Liang X. San3456ORCID,He Wei-Bang7

Affiliation:

1. a State Key Laboratory of Marine Environmental Science, College of Ocean and Earth Sciences, Xiamen University, Xiamen, China

2. b Department of Physical Oceanography, College of Ocean and Earth Sciences, Xiamen University, Xiamen, China

3. c Artificial Intelligence Department, Division of Frontier Research, Southern Marine Laboratory, Zhuhai, China

4. d CMA–FDU Joint Laboratory of Marine Meteorology, Department of Atmospheric and Oceanic Sciences, Fudan University, Shanghai, China

5. e Institute of Atmospheric Sciences, Fudan University, Shanghai, China

6. f IRDR ICoE on Risk Interconnectivity and Governance on Weather/Climate Extremes Impact and Public Health, Fudan University, Shanghai, China

7. g Department of Atmospheric Sciences, School of Ocean and Earth Science and Technology, University of Hawai‘i at Mānoa, Honolulu, Hawaii

Abstract

Abstract Motivated by the observation that the interannual variability of the North Atlantic Oscillation (NAO) is associated with the ensemble emergence of individual NAO events occurring on the intraseasonal time scale, one naturally wonders how the intraseasonal processes cause the interannual variability and what the dynamics are underlying the multiscale interaction. Using a novel time-dependent and spatially localized multiscale energetics formalism, this study investigates the dynamical sources for the NAO events with different phases and interannual regimes. For the positive-phase events (NAO+), the intraseasonal-scale kinetic energy (K1) over the North Atlantic sector is significantly enhanced for NAO+ occurring in the negative NAO winter regime (NW), compared to those in the positive winter regime (PW). It is caused by the enhanced inverse cascading from synoptic transients and reduced energy dispersion during the life cycle of NAO+ in NW. For the negative-phase events (NAO), K1 is significantly larger during the early and decay stages of NAO in NW than that in PW, whereas the reverse occurs in the peak stage. Inverse cascading and baroclinic energy conversion are primary drivers in the formation of the excessive K1 during the early stage of NAO in NW, whereas only the latter contributes to the larger K1 during the decay stage of NAO in NW compared to that in PW. The barotropic transfer from the mean flow, inverse cascading, and baroclinic energy conversion are all responsible for the strengthened K1 in the peak stage of NAO in PW.

Funder

National Science Foundation of China

Publisher

American Meteorological Society

Subject

Atmospheric Science

Reference76 articles.

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