×ばつ 10<sup>−3</sup> s<sup>−1</sup> during its lifetime of 54 min. The vortex initialized and remained inside the region of extreme rain rates (radar-retrieved rain rates > 100 mm h<sup>−1</sup>), reached its peak intensity after the peak of the collocated 6-min rainfall accumulation, and then weakened rapidly after the extreme rainfall region moved away. The radar-retrieved liquid water path was about five to seven times the ice water path and the specific differential phase (<i>K</i><sub>dp</sub>) below 0°C increased sharply downward during the lifetime of the vortex, suggesting the presence of active warm rain microphysical processes. These results indicate that the release of the latent heat of condensation induced by extreme rainfall could have contributed to the formation of the vortex in an environment with a weak 0–1-km vertical wind shear (about 4–5 m s<sup>−1</sup>) through enhanced low-level convergence, although the strengthening of low-level updrafts by rotational dynamic effects and short-term rainfall cannot be ruled out." /> ×ばつ 10<sup>−3</sup> s<sup>−1</sup> during its lifetime of 54 min. The vortex initialized and remained inside the region of extreme rain rates (radar-retrieved rain rates > 100 mm h<sup>−1</sup>), reached its peak intensity after the peak of the collocated 6-min rainfall accumulation, and then weakened rapidly after the extreme rainfall region moved away. The radar-retrieved liquid water path was about five to seven times the ice water path and the specific differential phase (<i>K</i><sub>dp</sub>) below 0°C increased sharply downward during the lifetime of the vortex, suggesting the presence of active warm rain microphysical processes. These results indicate that the release of the latent heat of condensation induced by extreme rainfall could have contributed to the formation of the vortex in an environment with a weak 0–1-km vertical wind shear (about 4–5 m s<sup>−1</sup>) through enhanced low-level convergence, although the strengthening of low-level updrafts by rotational dynamic effects and short-term rainfall cannot be ruled out." /> ×ばつ 10<sup>−3</sup> s<sup>−1</sup> during its lifetime of 54 min. The vortex initialized and remained inside the region of extreme rain rates (radar-retrieved rain rates > 100 mm h<sup>−1</sup>), reached its peak intensity after the peak of the collocated 6-min rainfall accumulation, and then weakened rapidly after the extreme rainfall region moved away. The radar-retrieved liquid water path was about five to seven times the ice water path and the specific differential phase (<i>K</i><sub>dp</sub>) below 0°C increased sharply downward during the lifetime of the vortex, suggesting the presence of active warm rain microphysical processes. These results indicate that the release of the latent heat of condensation induced by extreme rainfall could have contributed to the formation of the vortex in an environment with a weak 0–1-km vertical wind shear (about 4–5 m s<sup>−1</sup>) through enhanced low-level convergence, although the strengthening of low-level updrafts by rotational dynamic effects and short-term rainfall cannot be ruled out." />
Article views:
PDF downloads:
Cited by:
/