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A STUDY OF SIMPLIFIED SHALLOW WATER WAVES: ASSESSMENT OF ADOMIAN’S DECOMPOSITION METHOD<br />
FOR THE ANALYTICAL SOLUTION<br />
Mehdi Safari<br />
L u L u 3uL u 3L u L udx L u,<br />
(35)<br />
t<br />
where<br />
xxt<br />
t<br />
3<br />
<br />
<br />
L t<br />
, L x<br />
, L xxt<br />
,<br />
2<br />
t x x<br />
t<br />
x<br />
x<br />
t<br />
x<br />
(36)<br />
The terms u0 ( x,<br />
t),<br />
u1(<br />
x,<br />
t),<br />
u2<br />
( x,<br />
t)<br />
<strong>in</strong> Eq.44, obta<strong>in</strong>ed from<br />
Eqs.41, 42, 43. If we assume c=2 then by draw<strong>in</strong>g 3-D figures of ADM<br />
solutions. In Fig.2 the second model of shallow water wave equation<br />
with the first <strong>in</strong>itial condition (31) of Eq. (2) when c=2 has been shown.<br />
Fig.1. For the first model of shallow water wave equation with the first<br />
<strong>in</strong>itial condition (31) of Eq. (2), ADM result for u ( x,<br />
t)<br />
, when c=2.<br />
If the <strong>in</strong>vertible operator<br />
L L u L<br />
1<br />
t<br />
t<br />
1<br />
t<br />
( L<br />
xxt<br />
L<br />
1<br />
t<br />
t<br />
dt<br />
u 3uL u 3L u<br />
t<br />
0<br />
x<br />
is applied to Eq. 45, then<br />
<br />
x<br />
L udx L u),<br />
t<br />
x<br />
(37)<br />
is obta<strong>in</strong>ed. By this<br />
u(<br />
x,<br />
t)<br />
u(<br />
x,0)<br />
L<br />
1<br />
t<br />
( L<br />
xxt<br />
u 3uL u 3L u<br />
t<br />
x<br />
<br />
x<br />
L udx L u),<br />
t<br />
x<br />
(38)<br />
is found. Here the ma<strong>in</strong> po<strong>in</strong>t is that the solution of the decomposition<br />
method is <strong>in</strong> the <strong>form</strong> of<br />
u ( x,<br />
t)<br />
un<br />
( x,<br />
t)<br />
, (39)<br />
n0<br />
Substitut<strong>in</strong>g from Eq. 49 <strong>in</strong> 48, we f<strong>in</strong>d<br />
Fig.2. For the second model of shallow water wave equation with the<br />
first <strong>in</strong>itial condition (31) of Eq. (3), ADM result for u ( x,<br />
t)<br />
, when<br />
c=2.<br />
<br />
<br />
n0<br />
<br />
<br />
<br />
<br />
L ( , ) 3 ( , ) ( , )<br />
1<br />
0<br />
0<br />
0<br />
( , ) ( ,0)<br />
<br />
<br />
<br />
xxtun<br />
x t un<br />
x t Lt<br />
un<br />
x t <br />
n<br />
n<br />
n<br />
<br />
u<br />
n<br />
x t u x Lt<br />
<br />
, (40)<br />
<br />
x<br />
<br />
<br />
<br />
3 ( , ) ( , )<br />
( , ) <br />
Lx<br />
un<br />
x t <br />
Lt<br />
un<br />
x t dx<br />
Lx<br />
un<br />
x t <br />
n0<br />
n0<br />
n0<br />
<br />
is found.<br />
Accord<strong>in</strong>g to Eq.19 approximate solution can be obta<strong>in</strong>ed as follows:<br />
<br />
2 1 c 1<br />
<br />
( c 1)sech<br />
x<br />
2 c<br />
u0<br />
( x,<br />
t)<br />
<br />
<br />
,<br />
2c<br />
1 c 1<br />
c 1<br />
( c 1)s<strong>in</strong>h<br />
<br />
x<br />
2<br />
t<br />
1(<br />
, )<br />
c c<br />
x t <br />
,<br />
<br />
3 1 c 1<br />
<br />
2ccosh<br />
<br />
x<br />
2<br />
c <br />
(41)<br />
u (42)<br />
t<br />
<br />
(43)<br />
u2( x,<br />
t)<br />
( Lxxtu1<br />
3u1L tu1<br />
3Lxu1<br />
Lt<br />
u1dx<br />
Lxu1<br />
) dt,<br />
0<br />
Thus the approximate solution for second model of shallow water wave<br />
equation is obta<strong>in</strong>ed as<br />
u( x,<br />
t)<br />
u0 ( x,<br />
t)<br />
u1(<br />
x,<br />
t)<br />
u2<br />
( x,<br />
t)<br />
, (44)<br />
x<br />
CONCLUSION<br />
In this paper, Adomian’s decomposition method has been successfully<br />
applied to f<strong>in</strong>d the solution of two model equations for shallow water<br />
waves. The obta<strong>in</strong>ed results were showed graphically it is proved that<br />
Adomian's decomposition method is a powerful method for solv<strong>in</strong>g<br />
these equations. In our work; we used the Maple Package to calculate<br />
the functions obta<strong>in</strong>ed from the Adomian’s decomposition method.<br />
<strong>Academy</strong><strong>Publish</strong>.org – Journal of Eng<strong>in</strong>eer<strong>in</strong>g and Technology Vol.2, No.2 19