2006
DOI: 10.3319/tao.2006.17.2.429(a)
|View full text |Cite
|
Sign up to set email alerts
|

Doppler Velocity Signatures of Idealized Elliptical Vortices

Abstract: TAO, Vol. 17, No. 2, June 2006 430 can be seen that when the phase of the wavenumber two V T is ahead of V R by π/4 with same amplitude, GBVTD coefficients A3 and B3 are near zero; hence, GBVTD technique cannot retrieve the wavenumber two amplitude in these conditions. However, by knowing the elliptical shape of the vortex as a priori these two mechanisms can still be distinguished by the characteristics of the corresponding GBVTD coefficients.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2009
2009
2024
2024

Publication Types

Select...
5
1

Relationship

2
4

Authors

Journals

citations
Cited by 10 publications
(1 citation statement)
references
References 24 publications
(46 reference statements)
0
1
0
Order By: Relevance
“…6f), the shape of the wind speed distribution is elliptic, in contrast to the more circular shape of the reflectivity distribution. The ellipticity may be due to the presence of an azimuthal wavenumber two vortex Rossby wave propagating on the azimuthal mean vorticity gradient (Montgomery and Kallenbach 1997;Lee et al 2006). The presence of a wavenumber-2 perturbation is consistent with the barotropically unstable ring vorticity structure (shown in Fig.…”
Section: B Kinematic Structurementioning
confidence: 71%
“…6f), the shape of the wind speed distribution is elliptic, in contrast to the more circular shape of the reflectivity distribution. The ellipticity may be due to the presence of an azimuthal wavenumber two vortex Rossby wave propagating on the azimuthal mean vorticity gradient (Montgomery and Kallenbach 1997;Lee et al 2006). The presence of a wavenumber-2 perturbation is consistent with the barotropically unstable ring vorticity structure (shown in Fig.…”
Section: B Kinematic Structurementioning
confidence: 71%