multiscale interaction
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2021 ◽  
Author(s):  
Asmeret Naugle ◽  
Casey Doyle ◽  
Matthew Sweitzer ◽  
Fredrick Rothganger ◽  
Stephen Verzi ◽  
...  

Eos ◽  
2020 ◽  
Vol 101 ◽  
Author(s):  
Michel Boufadel ◽  
Scott Socolofsky

Exploring how the multiscale interaction between underwater oil and gas plumes and the environment impacts plume composition and trajectory.


2020 ◽  
Vol 77 (4) ◽  
pp. 1387-1414
Author(s):  
Dehai Luo ◽  
Yao Ge ◽  
Wenqi Zhang ◽  
Aiguo Dai

Abstract In this paper, reanalysis data are first analyzed to reveal that the individual negative (positive)-phase Pacific–North American pattern (PNA) or PNA− (PNA+) has a lifetime of 10–20 days, is characterized by strong (weak) westerly jet stream meanders, and exhibits clear wave train structures, whereas the PNA− with rapid retrogression tends to have longer lifetime and larger amplitude than the PNA+ with slow retrogression. In contrast, the wave train structure of the North Atlantic Oscillation (NAO) is less distinct, and the positive (negative)-phase NAO shows eastward (westward) movement around a higher latitude than the PNA. Moreover, it is found that the PNA wave train occurs under a larger background meridional potential vorticity gradient (PVy) over the North Pacific than that over the North Atlantic for the NAO. A unified nonlinear multiscale interaction (UNMI) model is then developed to explain why the PNA as a nonlinear wave packet has such characteristics and its large difference from the NAO. The model results reveal that the larger background PVy for the PNA (due to its location at lower latitudes) leads to its larger energy dispersion and weaker nonlinearity than the NAO, thus explaining why the PNA (NAO) is largely a linear (nonlinear) process with a strong (weak) wave train structure, though it is regarded as a nonlinear initial-value problem. The smaller PVy for the PNA− than for the PNA+ leads to lower energy dispersion and stronger nonlinearity for PNA−, which allows it to maintain larger amplitude and have a longer lifetime than the PNA+. Thus, the difference in the background PVy is responsible for the asymmetry between the two phases of PNA and the difference between the PNA and NAO.


2019 ◽  
Vol 76 (8) ◽  
pp. 2399-2427 ◽  
Author(s):  
Dehai Luo ◽  
Wenqi Zhang ◽  
Linhao Zhong ◽  
Aiguo Dai

Abstract In this paper, an extended nonlinear multiscale interaction model of blocking events in the equivalent barotropic atmosphere is used to investigate the effect of a slowly varying zonal wind in the meridional direction on dipole blocking that is regarded as a nonlinear Rossby wave packet. It is shown that the meridional gradient of potential vorticity (PVy=∂PV/∂y) prior to the blocking onset, which is related to the background zonal wind and its nonuniform meridional shear, can significantly affect the lifetime, intensity, and north–south asymmetry of dipole blocking, while the blocking dipole itself is driven by preexisting incident synoptic-scale eddies. The magnitude of the background PVy determines the energy dispersion and nonlinearity of blocking. It is revealed that a small background PVy is a prerequisite for strong and long-lived eddy-driven blocking that behaves as a persistent meandering westerly jet stream, while the blocking establishment further reduces the PVy within the blocking region, resulting in a positive feedback between blocking and PVy. When the core of the background westerly jet shifts from higher to lower latitudes, the blocking shows a northwest–southeast-oriented dipole with a strong anticyclonic anomaly to the northwest and a weak cyclonic anomaly to the southeast as its northern pole moves westward more rapidly and has weaker energy dispersion and stronger nonlinearity than its southern pole because of the smaller PVy in higher latitudes. The opposite is true when the background jet shifts toward higher latitudes. The asymmetry of dipole blocking vanishes when the background jet shows a symmetric double-peak structure. Thus, a small prior PVy is a favorable precursor for the occurrence of long-lived and large-amplitude blocking.


Author(s):  
Vladimir V. Makarov ◽  
Srilena Kundu ◽  
Daniil V. Kirsanov ◽  
Nikita S. Frolov ◽  
Vladimir A. Maksimenko ◽  
...  

2019 ◽  
Vol 19 (4) ◽  
pp. 333
Author(s):  
Yi Sai Gao ◽  
Guan Bang Wang ◽  
Ya Ting Xiao ◽  
Jia Qi Sun ◽  
Qiu yun Zheng ◽  
...  

2019 ◽  
Vol 19 (4) ◽  
pp. 333
Author(s):  
Xin Rong Zhang ◽  
Yi Sai Gao ◽  
Guan Bang Wang ◽  
Ya Ting Xiao ◽  
Jia Qi Sun ◽  
...  

2018 ◽  
Vol 58 (3) ◽  
pp. 039501
Author(s):  
M.J. Choi ◽  
J. Kim ◽  
J.-M. Kwon ◽  
H.K. Park ◽  
Y. In ◽  
...  

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