A nonlinear Schrödinger equation for the envelope of two dimensional surface water waves on finite depth with non-zero constant vorticity is derived, and the influence of this constant vorticity on the well-known stability properties of weakly nonlinear wave packets is studied. It is demonstrated that vorticity modifies significantly the modulational instability properties of weakly nonlinear plane waves, namely the growth rate and bandwidth. At third order, we have shown the importance of the nonlinear coupling between the mean flow induced by the modulation and the vorticity. Furthermore, it is shown that these plane wave solutions may be linearly stable to modulational instability for an opposite shear current independently of the dimensionless parameter kh, where k and h are the carrier wavenumber and depth, respectively.

1.
S.
Tsao
, “
Behaviour of surface waves on a linearly varying current
,”
Tr. Mosk. Fiz. Tekh. Inst. Issled. Mekh. Prikl. Mat.
3
,
66
84
(
1959
).
2.
R. A.
Dalrymple
, “
A finite amplitude wave on a linear shear current
,”
J. Geophys. Res.
79
,
4498
4504
, doi: (
1974
).
3.
I.
Brevik
, “
Higher-order waves propagating on constant vorticity currents in deep water
,”
Coastal Eng.
2
,
237
259
(
1979
).
4.
J. A.
Simmen
and
P. G.
Saffman
, “
Steady deep-water waves on a linear shear current
,”
Stud. Appl. Math.
73
,
35
57
(
1985
).
5.
A. F.
Teles
,
Da
Silva
, and
D. H.
Peregrine
, “
Steep, steady surface waves on water of finite depth with constant vorticity
,”
J. Fluid Mech.
195
,
281
302
(
1988
).
6.
N.
Kishida
and
R. J.
Sobey
, “
Stokes theory for waves on linear shear current
,”
J. Eng. Mech.
114
,
1317
1334
(
1988
).
7.
O. S.
Pak
and
K. W.
Chow
, “
Free surface waves on shear currents with non-uniform vorticity: Third order solutions
,”
Fluid Dyn. Res.
41
,
1
13
(
2009
).
8.
A.
Constantin
, “
Two-dimensionality of gravity water flows of constant non zero vorticity beneath a surface wave train
,”
Eur. J. Mech. B/Fluids
30
,
12
16
(
2011
).
9.
D. H.
Peregrine
, “
Interaction of water waves and currents
,”
Adv. Appl. Mech.
16
,
9
117
(
1976
).
10.
I. G.
Jonsson
, “
Wave-current interactions
,” in
The Sea
(
Wiley
,
New York
,
1990
), pp.
65
120
.
11.
G. P.
Thomas
and
G.
Klopman
, “
Wave-current interactions in the near shore region
,” in
Gravity Waves in Water of Finite Depth
, edited by
J. N.
Hunt
(
Computational Mechanics
,
Southampton
,
1997
), pp.
215
319
.
12.
R. S.
Johnson
, “
On the modulation of water waves on shear flows
,”
Proc. R. Soc. London, Ser. A
347
,
537
546
(
1976
).
13.
M.
Oikawa
,
K.
Chow
, and
D. J.
Benney
, “
The propagation of nonlinear wave packets in a shear flow with a free surface
,”
Stud. Appl. Math.
76
,
69
92
(
1987
).
14.
J. C.
Li
,
W. H.
Hui
, and
M. A.
Donelan
, “
Effects of velocity shear on the stability of surface deep water wave trains
,” in
Nonlinear Water Waves
, edited by
K.
Horikawa
and
H.
Maruo
(
Springer
,
Berlin
,
1987
), pp.
213
220
.
15.
A. I.
Baumstein
, “
Modulation of gravity waves with shear in water
,”
Stud. Appl. Math.
100
,
365
390
(
1998
).
16.
W.
Choi
, “
Nonlinear surface waves interacting with a linear shear current
,”
Math. Comput. Simul.
80
,
101
110
(
2009
).
17.
M.
Okamura
and
M.
Oikawa
, “
The linear stability of finite amplitude surface waves on a linear shearing flow
,”
J. Phys. Soc. Jpn.
58
,
2386
2396
(
1989
).
18.
A.
Davey
and
K.
Stewartson
, “
On three-dimensional packets of surface waves
,”
Proc. R. Soc. London, Ser. A
338
,
101
110
(
1974
).
19.
P. A. E. M.
Janssen
, “
Nonlinear four-wave interactions and freak waves
,”
J. Phys. Oceanogr.
33
,
863
884
(
2003
).
20.
M.
Onorato
,
A. R.
Osborne
,
M.
Serio
,
L.
Cavaleri
,
C.
Brandini
, and
C. T.
Stansberg
, “
Extreme waves, modulational instability and second order theory: Wave flume experiments on irregular waves
,”
Eur. J. Mech. B/Fluids
25
,
586
601
(
2006
).
21.
C.
Kharif
,
E.
Pelinovsky
, and
A.
Slunyaev
,
Rogue Waves in the Ocean
(
Springer
,
Heidelberg
,
2009
).
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