A detailed linear stability analysis of an easterly barotropic Gaussian jet centered at the equator is performed in the long-wave sector in the framework of one- and two-layer shallow-water models on the equatorial β-plane. It is shown that the dominant instability of the jet is due to phase-locking and resonance between Yanai waves, although the standard barotropic and baroclinic instabilities due to the resonance between Rossby waves are also present. In the one-layer case, this dominant instability has non-zero growth rate at zero wavenumber for high enough Rossby and low enough Burger numbers, thus reproducing the classical symmetric inertial instability. Yet its asymmetric counterpart has the highest growth rate. In the two-layer case, the dominant instability may be barotropic or baroclinic, the latter being stronger, with the maximum of the growth rate shifting towards smaller downstream wavenumbers as Rossby number increases at fixed Burger number, and given thickness and density ratios. At large enough Rossby numbers this instability has a non-zero growth rate limit at zero wavenumber, giving the baroclinic symmetric inertial instability. Again, the maximal growth rate is achieved at small but non-zero wavenumbers, corresponding to the asymmetric inertial instability. At high enough Rossby number and low enough Burger number not only the baroclinic, but also the barotropic symmetric instability appears, as well as higher meridional modes of the baroclinic symmetric instability. Still, all of them are dominated by their asymmetric counterparts. Direct numerical simulations of the saturation of the leading instabilities are performed, showing that the barotropic species of the instability saturates by forming a double vortex street subject to nonlinear oscillations, while the baroclinic, the most vigorous one, saturates by producing strong vertical shears and related dissipation and mixing.

1.
S. G. H.
Philander
, “
Instabilities of zonal equatorial currents
,”
J. Geophys. Res.
81
,
3725
3735
, doi: (
1976
).
2.
P.
Chatterjee
and
B. N.
Goswami
, “
Structure, genesis and scale selection of the tropical quasi-biweekly mode
,”
Q. J. R. Met. Soc.
130
,
1171
(
2004
).
3.
J. L.
Mitchell
and
G. K.
Vallis
, “
The transition to superrotation in terrestrial atmospheres
,”
J. Geophys. Res.
115
,
E12008
, doi: (
2010
).
4.
B. L.
Hua
,
D. W.
Moore
, and
S.
Le Gentil
, “
Inertial nonlinear equilibration of equatorial flows
,”
J. Fluid Mech.
331
,
345
371
(
1997
).
5.
S. D.
Griffiths
, “
The nonlinear evolution of zonally symmetric equatorial inertial instability
,”
J. Fluid Mech.
474
,
245
273
(
2003
).
6.
F.
Bouchut
,
B.
Ribstein
, and
V.
Zeitlin
, “
Inertial, barotropic, and baroclinic instabilities of the Bickley jet in two-layer rotating shallow water model
,”
Phys. Fluids
23
,
126601
(
2011
).
7.
G. F.
Carnevale
,
R. C.
Kloosterziel
, and
P.
Orlandi
, “
Inertial and barotropic instabilities of a free current in three-dimensional rotating flow
,”
J. Fluid Mech.
725
,
117
151
(
2013
).
8.
B.
Ribstein
,
R.
Plougonven
, and
V.
Zeitlin
, “
Inertial vs baroclinic instability of the Bickley jet in continuously stratified fluid
,”
J. Fluid Mech.
743
,
1
31
(
2014
).
9.
J. P.
Holton
,
An Introduction to Dynamic Meteorology
(
Academic Press
,
NY
,
1992
).
10.
A.
Gill
, “
Some simple solutions for heat-induced tropical circulation
,”
Q. J. R. Met. Soc.
106
,
447
462
(
1980
).
11.
D. A.
Schecter
and
T. J.
Dunkerton
, “
Hurricane formation in diabatic Ekman turbulence
,”
Q. J. R. Met. Soc.
135
,
823
838
(
2009
).
12.
A.
Gill
,
Atmosphere-Ocean Dynamics
(
Academic Press
,
London
,
1982
).
13.
F.
Bouchut
and
V.
Zeitlin
, “
A robust well-balanced scheme for multi-layer shallow water equations
,”
Disc. Cont. Dyn. Syst. B
13
,
739
758
(
2010
).
14.
Y.-Y.
Hayashi
and
W. R.
Young
, “
Stable and unstable shear modes of rotating parallel flows in shallow water
,”
J. Fluid Mech.
184
,
477
504
(
1987
).
15.
M.
Renardy
and
J.
Swaters
, “
Stability of equatorial currents with nonzero potential vorticity
,”
Geophys. Astrophys. Fluid Dyn.
85
,
31
64
(
1997
).
16.
H.
Taniguchi
and
M.
Ishiwatari
, “
Physical interpretation of unstable modes of a linear shear flow in shallow water on an equatorial beta-plane
,”
J. Fluid Mech.
567
,
1
26
(
2006
).
17.
S.-I.
Iga
and
Y.
Matsuda
, “
Shear instability in a shallow water model with implications for the venus atmosphere
,”
J. Atmos. Sci.
62
,
2514
2527
(
2005
).
18.
R. C.
Kloosterziel
,
P.
Orlandi
, and
G. F.
Carnevale
, “
Saturation of equatorial inertial instability
,” personal communication (
2014
).
19.
V.
Zeitlin
, in
Nonlinear Dynamics of Rotating Shallow Water: Methods and Advances
, edited by
V.
Zeitlin
(
Elsevier
,
Amesterdam
,
2007
).
20.
M.
Wheeler
and
G. N.
Kiladis
, “
Convectively coupled equatorial waves: Analysis of clouds and temperature in the wavenumber-frequency domain
,”
J. Atmos. Sci.
56
,
374
399
(
1999
).
21.
J.
Le Sommer
,
H.
Teitelbaum
, and
V.
Zeitlin
, “
Global estimates of equatorial inertia-gravity wave activity in the stratosphere inferred from ERA40 reanalysis
,”
Geophys. Res. Lett.
33
,
L07810
, doi: (
2006
).
22.
J.-I.
Yano
and
M.
Bonazzola
, “
Scale analysis for large-scale tropical atmospheric dynamics
,”
J. Atmos. Sci.
66
,
159
172
(
2009
).
23.
S. D.
Griffiths
, “
The limiting form of inertial instability in geophysical flows
,”
J. Fluid Mech.
605
,
115
143
(
2008
).
24.
P.
Ripa
, “
General stability conditions for a multi-layer model
,”
J. Fluid Mech.
222
,
119
137
(
1991
).
25.
L. N.
Trefethen
,
Spectral Methods in Matlab
(
SIAM
,
Philadelphia
,
2000
).
26.
V.
Zeitlin
,
S. B.
Medvedev
, and
R.
Plougonven
, “
Frontal geostrophic adjustment, slow manifold and nonlinear wave phenomena in one-dimensional rotating shallow water. Part 1. Theory
,”
J. Fluid Mech.
481
,
269
290
(
2003
).
27.
R.
Plougonven
and
V.
Zeitlin
, “
Nonlinear development of inertial instability in a barotropic shear
,”
Phys. Fluids
21
,
106601
(
2009
).
28.
F.
Bouchut
,
J.
Le Sommer
, and
V.
Zeitlin
, “
Breaking of equatorial waves
,”
Chaos
15
,
013503
(
2005
).
29.
F. L.
Poulin
and
G. R.
Flierl
, “
The nonlinear evolution of barotropically unstable jets
,”
J. Phys. Oceanogr.
33
,
2173
2192
(
2003
).
30.
J.
Lambaerts
,
G.
Lapeyre
, and
V.
Zeitlin
, “
Moist vs dry barotropic instability in a shallow water model of the atmosphere with moist convection
,”
J. Atmos. Sci.
68
,
1234
1252
(
2011
).
31.
S.
Sakai
, “
Rossby-Kelvin instability: A new type of ageostrophic instability caused by a resonance between Rossby waves and gravity waves
,”
J. Fluid Mech.
202
,
149
176
(
1989
).
32.
T. J.
Dunkerton
, “
A nonsymmetric equatorial inertial instability
,”
J. Atmos. Sci.
38
,
807
813
(
1982
).
33.
F.
Bouchut
, in
Nonlinear Dynamics of Rotating Shallow Water: Methods and Advances
, edited by
V.
Zeitlin
(
Elsevier
,
Amesterdam
,
2007
).
34.
J.
Le Sommer
,
S. B.
Medvedev
,
R.
Plougonven
, and
V.
Zeitlin
, “
Singularity formation during relaxation of jets and fronts toward the state of geostrophic equilibrium
,”
Commun. Nonlin. Sci. Num. Simul.
8
,
415
442
(
2003
).
35.
R. C.
Kloosterziel
,
P.
Orlandi
, and
G. F.
Carnevale
, “
Saturation of inertial instability in rotating planar shear flows
,”
J. Fluid Mech.
583
,
413
422
(
2007
).
36.
D. E.
Stevens
and
P. E.
Ciesielski
, “
Inertial instability of horizontally sheared flow away from the equator
,”
J. Atmos. Sci.
43
,
2845
2856
(
1986
).
You do not currently have access to this content.