Abstract

Using the four-times daily and monthly-mean reanalysis datasets of NCEP/NCAR for the 1958 to 2018 period, we investigate the interannual variability of the June-July-August (JJA)–mean water vapor source and sink over the tropical eastern Indian Ocean-Western Pacific (TEIOWP) and the underlying mechanism. It is found that the two major modes (EOF1 and EOF2) of the water vapor source and sink anomalies over the TEIOWP present a southwest-northeast oriented dipole and a southwest-northeast oriented tripole. Specifically, when the western maritime continent shows an anomalous water vapor source, the northwestern Pacific is characterized by anomalous water vapor sink and source in EOF1 and EOF2 modes, respectively. The EOF1 and EOF2 modes are primarily driven by a single and a double meridional cell anomaly, which corresponds to the in-phase and out-of-phase linkage between evaporation anomalies over the western maritime continent and precipitation anomalies over the northwestern Pacific, respectively. Furthermore, the EOF1 mode is regulated by the quick transition of the El Niño-Southern Oscillation (ENSO) phase, whereas the EOF2 mode probably originates from internal atmospheric variability. Considering that the standard deviation of PC1 is much higher during ENSO years than that during non-ENSO years, it is probable that the water source and sink anomalies over the TEIOWP tend to be dominant by EOF1 mode during ENSO years. In contrast, the EOF2 mode may play an important role in the water source and sink anomalies over the TEIOWP during non-ENSO years. Accordingly, the water vapor source and sink anomalies over the TEIOWP may be well predicted based on the ENSO state in the previous December-January-February. These results are useful for understanding the predictability of water vapor source and sink anomalies over the TEIOWP.

Highlights

  • The water vapor in the atmosphere accounts for only 0.001% of the global water, this tiny fraction is the most active part of the water cycle [1,2]

  • More than 25% and 12% of the total variance can be explained by the EOF1 and EOF2, which can be well separated from the other modes according to the “rule of thumb” [35]

  • (Figure 5b,d), we examine whether the EOF2 mode is affected by the tropical Indian Ocean dipole (TIOD) via the lead-lag correlations

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Summary

Introduction

The water vapor in the atmosphere accounts for only 0.001% of the global water, this tiny fraction is the most active part of the water cycle [1,2]. The atmospheric water cycle mainly includes evaporation, water vapor transport and precipitation, linking water exchange among ocean, land and different regions. The water vapor is mostly concentrated in the lower atmosphere and decreases rapidly with the increase of altitude. The water vapor over the equator is abundant and it decreases significantly towards the North and South poles. As the central part of the warm pool, the tropical eastern Indian Ocean-western Pacific (TEIOWP) is the most abundant region of water vapor in the world [2,3].

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