Affiliation:
1. Brno University of Technology, Faculty of Civil Engineering, Department of Mathematics and Descriptive Geometry, Faculty of Electrical Engineering and Communication, Department of Mathematics , Brno , Czech Republic
2. Department of Mathematics, Faculty of Electrical Engineering and Communication, Brno University of Technology , Brno , Czech Republic
Abstract
Abstract
The article investigates a second-order nonlinear difference equation of Emden-Fowler type
Δ
2
u
(
k
)
±
k
α
u
m
(
k
)
=
0
,
{\Delta }^{2}u\left(k)\pm {k}^{\alpha }{u}^{m}\left(k)=0,
where
k
k
is the independent variable with values
k
=
k
0
,
k
0
+
1
,
…
k={k}_{0},{k}_{0}+1,\ldots \hspace{0.33em}
,
u
:
{
k
0
,
k
0
+
1
,
…
}
→
R
u:\left\{{k}_{0},{k}_{0}+1,\ldots \hspace{0.33em}\right\}\to {\mathbb{R}}
is the dependent variable,
k
0
{k}_{0}
is a fixed integer, and
Δ
2
u
(
k
)
{\Delta }^{2}u\left(k)
is its second-order forward difference. New conditions with respect to parameters
α
∈
R
\alpha \in {\mathbb{R}}
and
m
∈
R
m\in {\mathbb{R}}
,
m
≠
1
m\ne 1
, are found such that the equation admits a solution asymptotically represented by a power function that is asymptotically equivalent to the exact solution of the nonlinear second-order differential Emden-Fowler equation
y
″
(
x
)
±
x
α
y
m
(
x
)
=
0
.
{y}^{^{\prime\prime} }\left(x)\pm {x}^{\alpha }{y}^{m}\left(x)=0.
Two-term asymptotic representations are given not only for the solution itself but also for its first- and second-order forward differences as well. Previously known results are discussed, and illustrative examples are considered.
Cited by
3 articles.
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