We apply the theory of Weierstrass elliptic function to study exact solutions of the generalized Benjamin-Bona-Mahony equation. By using the theory of Weierstrass elliptic integration, we get some traveling wave solutions, which are expressed by the hyperbolic functions and trigonometric functions. This method is effective to find exact solutions of many other similar equations which have arbitrary-order nonlinearity

Lixin Tian

Xun Liu

Yuhai Wu

Mathematical Problems in Engineering

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Exact Solutions of the Generalized Benjamin-Bona-Mahony Equation

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Hindawi Publishing Corporation
Mathematical Problems in Engineering
Volume 2010, Article ID 796398, 5 pages
doi:10.1155/2010/796398
Research Article
Exact Solutions of the Generalized
Benjamin-Bona-Mahony Equation
Xun Liu, Lixin Tian, and Yuhai Wu
Faculty of Science, Jiangsu University, Zhenjiang, Jiangsu 212013, China
Correspondence should be addressed to Xun Liu, liuxundy@163.com
Received 5 February 2010; Revised 30 June 2010; Accepted 26 September 2010
Academic Editor: Yuri Vladimirovich Mikhlin
Copyright q 2010 Xun Liu et al. This is an open access article distributed under the Creative
Commons Attribution License, which permits unrestricted use, distribution, and reproduction in
any medium, provided the original work is properly cited.
We apply the theory of Weierstrass elliptic function to study exact solutions of the generalized
Benjamin-Bona-Mahony equation. By using the theory of Weierstrass elliptic integration, we get
some traveling wave solutions, which are expressed by the hyperbolic functions and trigonometric
functions. This method is eﬀective to find exact solutions of many other similar equations which
have arbitrary-order nonlinearity.
1. Introduction
The nonlinear phenomena in the scientific work or engineering fields are more and more
attractive to scientists. To depict and analyze such nonlinear phenomena, the nonlinear
evolutionary equations are playing an important role and their solitary wave solutions are
the main interests of mathematicians and physicists.
To obtain the traveling wave solutions of these nonlinear evolution equations, many
methods were attempted, such as the inverse scattering method, Hirota’s bilinear transfor-
mation, the tanh-sech method, extended tanh method, sine-cosine method, homogeneous
balance method, and exp-function method. With the aid of symbolic computation system,
many explicit solutions are easily obtained, and many interesting works deeply promote the
research of nonlinear phenomena.
The present work is interested in generalized Benjamin-Bona-Mahony BBM
equation:
ut  aux 
(
bun  cu2n
)
ux  kuxxx  0. 1.1
2 Mathematical Problems in Engineering
In the above equation, the first term of left side represents the evolution term while
parameters b and c represent the coeﬃcients of dual-power law nonlinearity, a and k are the
coeﬃcients of dispersion terms, n is the power law parameter, and variable u is the wave
profile. In 1	, Biswas used the solitary wave ansatz and obtained an exact 1-soliton solution
of 1.1. In order to find more exact solutions of some nonlinear evolutionary equations, the
Weierstrass elliptic function was introduced. For example, Kuru 2, 3	 discussed the BBM-like
equation, and Este´vez et al. 4	 analyzed another type of generalized BBM equations. In 5	,
Deng et al. also applied the similar method to the study of a nonlinear variant of the PHI-four
equation. In this paper, we will apply the method to the generalized Benjamin-Bona-Mahony
equation.
The rest of this paper is organized as follows. In Section 2, we first outline the
Weierstrass elliptic function method. In Section 3, we give exact expression of some traveling
wave solutions of generalized Benjamin-Bona-Mahony BBM equation 1.1 by using the
Weierstrass elliptic function method. Finally, some conclusions are given in Section 4.
2. Description of the Weierstrass Elliptic Function Method
When we search for the solutions of some evolutionary equations, we will meet the following
ordinary diﬀerential equation:
(
dϕ
dθ
)2
 P4
(
ϕ
)
 a0ϕ4  4a1ϕ3  6a2ϕ2  4a3ϕ  a4. 2.1
In 6	, Whittaker and Watson introduced two invariants:
g2  a0a4 − 4a1a3  3a22, g3  a0a2a4  2a1a2a3 − a32 − a0a23 − a21a4, 2.2
and a discriminant Δ  g32 − 27g23 ; then the solutions of diﬀerential 2.1 have the following
form:
ϕθ  ϕ0 
1
4
Pϕ
(
ϕ0
)(
℘
(
θ; g2, g3
) − 1
24
Pϕϕ
(
ϕ0
))−1
, 2.3
where ϕ0 is one of the roots of the polynomial P4ϕ, and Pϕϕ0, Pϕϕϕ0, respectively, denote
the first and second derivative of P4ϕ with respect to ϕ at the ϕ0. Particularly, if Δ  g32 −
27g23  0, then the Weierstrass elliptic function ℘θ; g2, g3 satisfies these conditions:
℘
(
θ; 12b2,−8b3
)
 b  3b sinh−2
(√
3bθ
)
,
℘
(
θ; 12b2, 8b3
)
 −b  3b sin−2
(√
3bθ
)
.
2.4
Once we get the solution of 2.1 with the form of 2.3, we will get the exact expressions of
solutions of many partial diﬀerential equations. Suppose that Δ  g32 − 27g23  0; it is obvious
that if g2 > 0, g3 > 0, then there exist period solutions of original evolutionary equation,
otherwise if g2 > 0, g3 < 0, then there exist solitary solutions.
Mathematical Problems in Engineering 3
3. Discussion on Generalized BBM Equation 1.1
Let ux, t  uξ, ξ  x − vt, so 1.1 is carried to
a − vu  b
n  1
un1 
c
2n  1
u2n1  ku′′  D, 3.1
where D is an integral constant. We introduce the transformation that
uξ 
(
kn  1
b
)1/n
Wξ, 3.2
so that 3.1 is changed to
W ′′ − v − a
k
W Wn1 
ckn  12
b22n  1
W2n1 
D
k
(
b
kn  1
)1/n
. 3.3
Let B  v − a/k, C  −ckn  12/b22n  1, and R1  D/kb/kn  11/n; then 3.3 is
transformed to the following form:
W ′′  BW −Wn1  CW2n1  R1. 3.4
By multiplying each side of 3.4 byW ′, integrating once again, we get that
(
W ′
)2  BW2 − 2
n  2
Wn2 
C
n  1
W2n2  2R1W  R2, 3.5
where R2 is the other integration constant.
LetW  ϕp; then the above equation is changed to
(
dϕ
dξ
)2

B
p2
ϕ2 − 2
n  2p2
ϕnp2 
C
n  1p2
ϕ2np2 
2R1
p2
ϕ2−p 
R2
p2
ϕ21−p. 3.6
Only if all the power of ϕ appearing in the right side of 3.6 are the integers and are
between 0 and 4, can we guarantee the integrability of 3.6. Therefore, if R1  R2  0, then
p  ±1/n. We choose the only case that if p  −1/n, then
(
dϕ
dξ
)2
 n2Bϕ2 − 2n
2
n  2
ϕ 
n2C
n  1
. 3.7
The polynomial Pϕ has two roots: ϕ0  n1±
√
n  1BCn  22  n  1	/Bn1n
2. For simplicity, let λ 
√
n  1BCn  22  n  1	, then ϕ0  n1±λ/Bn1n2
g2 
n4B2
12
, g3  −n
6B3
216
, Δ  0. 3.8
4 Mathematical Problems in Engineering
Then at the point ϕ0  n  1 ± λ/Bn  1n  2, the nonzero solutions of 3.7 are
℘
(
θ; g2, g3
)

n2B
12

1
4
n2B csch2
(√
B
2
nθ
)
, if B > 0,
℘
(
θ; g2, g3
)

n2B
12
− 1
4
n2B csc2
(√−B
2
nθ
)
, if B < 0.
3.9
The solutions of the ordinary diﬀerential equation are
ϕξ 
n  1 ±
[
λ − 2λ cosh2
((√
B/2
)
nθ
)]
Bn  1n  2
, if B > 0,
ϕξ 
n  1 ±
[
λ − 2λ cos2
((√−B/2
)
nθ
)]
Bn  1n  2
, if B < 0,
3.10
where B  v − a/k, C  −ckn  12/b22n  1, R1  D/kb/kn  11/n. Therefore, the
solutions of partial diﬀerential equation are
ux, t 
⎛
⎜⎝kn  1
b
Bn  1n  2
n  1 ±
[
λ − 2λ cosh2
((√
B/2
)
nθ
)]
⎞
⎟⎠
1/n
, if B > 0,
ux, t 
⎛
⎜⎝kn  1
b
Bn  1n  2
n  1 ±
[
λ − 2λ cos2
((√−B/2
)
nθ
)]
⎞
⎟⎠
1/n
, if B < 0,
3.11
where B  v − a/k,C  −ckn  12/b22n  1, and R1  D/kb/kn  11/n.
Remark 3.1. We have checked that 3.11 is the solution of 1.1. From the above discussion,
we find more solutions than the work of 1	.
4. Conclusions
From the above discussion, we find the traveling wave solutions of the generalized BBM
equation, which are expressed by the hyperbolic functions and trigonometric functions,
without the aid of symbolic computations. In addition, the method is eﬀective to find exact
solutions of many other similar equations which have arbitrary-order nonlinearity.
Acknowledgments
The authors would like to express their sincere thanks to referees for the valuable advice.
The present work was supported by the National Nature Science Foundation of China no.
10771088 and Foundation for Younger Personnel of Jiangsu University no. 1241190006.
Mathematical Problems in Engineering 5
References
1	 A. Biswas, “1-soliton solution of Benjamin-Bona-Mahoney equation with dual-power law nonlinear-
ity,” Communications in Nonlinear Science and Numerical Simulation, vol. 15, no. 10, pp. 2744–2746, 2010.
2	 S. Kuru, “Compactons and kink-like solutions of BBM-like equations bymeans of factorization,” Chaos,
Solitons and Fractals, vol. 42, no. 1, pp. 626–633, 2009.
3	 S¸. Kuru, “Traveling wave solutions of the BBM-like equations,” Journal of Physics A, vol. 42, no. 37,
Article ID 375203, 12 pages, 2009.
4	 P. G. Este´vez, S¸. Kuru, J. Negro, and L. M. Nieto, “Travelling wave solutions of the generalized
Benjamin-Bona-Mahony equation,” Chaos, Solitons and Fractals, vol. 40, no. 4, pp. 2031–2040, 2009.
5	 X. Deng, M. Zhao, and X. Li, “Travelling wave solutions for a nonlinear variant of the PHI-four
equation,”Mathematical and Computer Modelling, vol. 49, no. 3-4, pp. 617–622, 2009.
6	 E. T. Whittaker and G. N. Watson, A Course of Modern Analysis. An Introduction to the General Theory
of Infinite Processes and of Analytic Functions, Cambridge Mathematical Library, Cambridge University
Press, Cambridge, UK, 1996.
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