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Scientific Reports
| (2021) 11:13202 |
https://doi.org/10.1038/s41598-021-92548-7
www.nature.com/scientificreports/
the distorted cyclonic vortices, which is most prominent in midwinter. The result is qualitatively similar when a
non-zero curvature threshold is used (Supplementary Fig. S8).
Our method to identify cyclonic and anticyclonic vortices can be applied to storm tracks over other ocean
basins as well. Figures
3
c–d show westerly acceleration exerted by cyclonic and anticyclonic vortices, respec-
tively, over the North Atlantic (averaged over 80° − 50°W). In the lower troposphere, the westerly acceleration by
cyclonic vortices is much stronger, while it is slightly weaker in the upper troposphere than that by anticyclonic
vortices. Additionally, near-surface westerly deceleration by cyclonic vortices is striking along the southern
fringe (at ~ 60°N) of the semi-permanent Icelandic Low, especially in midwinter. These characteristics are in
common with the North Pacific storm track. Figures
3
e–f show the corresponding westerly acceleration over
the summertime South Indian Ocean (averaged over 75° − 105°E), where a distinct subpolar eddy-driven jet
forms at ~ 45°S. This situation resembles that over the summertime North Pacific. Lower-tropospheric westerly
acceleration by cyclonic vortices is much stronger than by anticyclonic vortices, while the contributions from
cyclonic and anticyclonic vortices are comparable in the upper troposphere. These features are consistent with
the two Northern Hemispheric oceanic storm tracks. Over the summertime South Indian Ocean, poleward
westerly momentum flux in the upper troposphere from the subtropics into the midlatitude jet core is striking
for both cyclonic and anticyclonic vortices.
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