Two Modified Three-Step Iterative Methods for Solving Nonlinear
Equations
Liang Fang
1
*, Rui Chen
1
and Jing Meng
1
1
College of Mathematics and Statistics, Taishan University, Tai'an, China
Keywords: Nonlinear equation, iterative method, Newton's method, efficiency index.
Abstract: With the rapid development of information and engineering technology and wide application of science and
technology, nonlinear problems become an important direction of research in the field of numerical
calculation and analysis. In this paper, we mainly study modified iterative methods for solving nonlinear
equations. We present and analyze a sixth-order convergent modified three-step Newton-type method for
solving nonlinear equations. Then we give a seventh-order convergence algorithm. The convergence
analysis of the presented algorithms are given. Both of the given methods are free from second derivatives.
The efficiency indices of the presented methods are 1.431 and 1.476, respectively, which are better than that
of the classical Newton’s method 1.414. Some numerical experiments illustrate the efficiency and
performance of the proposed two methods.
1 INTRODUCTION
Nonlinear problems are an important direction of
research in the field of numerical calculation and
analysis. The solution of nonlinear equations is one
of the most investigated topics in applied
mathematics, numerical analysis, and the problem of
solving nonlinear equations by numerical methods
has gained more importance than before, since many
practical problems in the applied information
technology, as well as in intelligent materials and
mechanical engineering, can build a suitable
mathematical model, and then be transformed into
nonlinear equations to solve.
In this paper, in order to improve the efficiency,
we consider iterative methods to find a simple root
of a nonlinear equation
() 0fx= , (1)
where
:
f
RRΩ⊆
for an open interval
Ω
is
a scalar function and it is sufficiently differentiable
in a neighborhood of
α
.
It is well known that the classical Newton's
method (NM) is an important and basic method for
solving nonlinear equation [1] by the iterative
scheme
1
()
'( )
n
nn
n
f
x
xx
f
x
+
=− (2)
which is quadratically convergent in the
neighborhood of
α
.
In recent years, much attention has been given to
develop iterative methods for solving nonlinear
equations and a vast literature has been produced [2-
12].
Motivated and inspired by the on-going activities
in this direction, in this paper, we present a sixth-
order convergent three-step iterative method and a
seventh-order convergent method. Both of the three-
step methods are free from second derivatives.
Several numerical results are given to illustrate the
efficiency and advantage of the algorithms.
2 TWO MODIFIED THREE-STEP
METHODS AND THEIR
CONVERGENCE ANALYSIS
Let us consider the following two three-step iterative
methods.
Algorithm 1. For given
0
x
, we consider the
following iteration scheme
()
'( )
n
nn
n
f
x
yx
f
x
=−
(3)
2
2( ) ( ) '( )
,
'( )
'( )
nnn
nn
n
n
f
yfyfy
zy
fx
fx
=− + (4)
22
1
22
5'( ) 3'( ) ( )
.
'( )
'( ) 7 '( )
nnn
nn
n
nn
xfyfz
xz
f
x
fx fy
+
+
=−
+
(5)
For Algorithm 1, we have the following
convergence result.
THEOREM 1. Assume that the function
:
f
RRΩ⊆ has a single root
α
∈Ω
, where
Ω is an open interval. If ()
f
x has first, second
and third derivatives in the interval
Ω , then
Algorithm 1 defined by (3)-(5) is sixth-order
convergent in a neighborhood of
α
and it satisfies
error equation
56 7
12
5()
nnn
eceOe
+
=+ (6)
where
,
nn
ex
α
=−
(7)
()
()
,1,2,
!'()
k
k
f
ck
kf
α
α
==L . (8)
Proof. Let
α
be the simple root of ()
f
x , and
()
()
,1,2,
!'()
k
k
f
ck
kf
α
α
==L
nn
ex
α
=−.
Consider the iteration function ()Fx defined by
22
22
5'() 3'(()) (())
() ()
'( )
'( ) 7 '( ( ))
f
xfyxfzx
Fx zx
f
x
fx fyx
+
=−
+
(9)
where
By some computations using Maple we can
obtain
()
( ) , ( ) 0, 1,2,3,4,5,
i
FF i
αα α
===
(10)
(11)
Further more, from the Taylor expansion of
()
n
Fx
around
α
, we get
(4) (5)
45
(6)
67
() ()
() ()
4! 5!
()
()(()).
6!
nn
nn
FF
xx
F
xOx
αα
αα
α
αα
+−+−
+−+
(12)
Substituting (11) into (12) yields
56 7
112
5().
nn nn
x
eceOe
αα
++
=+ =+ +
Therefore, we have
56 7
12
5()
nnn
eceOe
+
=+
which shows that Algorithm 1 defined by (3)-(5)
is sixth-order convergent.
Algorithm 2. For given
0
x
, we consider the
three-step Newton-type iteration scheme
()
'( )
n
nn
n
f
x
yx
f
x
=−
(13)
2
2( ) ( ) '( )
,
'( )
'( )
nnn
nn
n
n
f
yfyfy
zy
fx
fx
=− +
(14)
1
'( ) '( ) ( )
.
'( ) 3 '( ) '( )
nnn
nn
nnn
f
xfyfz
xz
f
xfyfx
+
+
=−
−+
(15)
THEOREM 2. Assume that the function
:
f
RRΩ⊆
has a single root
α
∈Ω
, where
Ω
is an open interval. If
()
f
x
has first, second
(2) 5
(6)
5
225 ( )
() .
2'()
f
F
f
α
α
α
=
1
(2) (3)
23
() () '()( )
() ()
() ()
2! 3!
nn n
nn
xFxFFx
FF
xx
ααα
αα
αα
+
==+
+−+
2
2 (()) (()) '(())
() () ,
'( )
'( )
()
() .
'( )
f
yx f yx f yx
zx yx
fx
fx
fx
yx x
fx
=− +
=−
and third derivatives in the interval
Ω
, then
Algorithm 2 is seventh-order convergent in a
neighborhood of
α
and it satisfies error equation
42 7 8
1223
10 ( ) ( )
nnn
eccceOe
+
=−+,
where
,
nn
ex
α
=−
()
()
,1,2,
!'()
k
k
f
ck
kf
α
α
==L .
Proof. Let
α
be the simple root of
()
f
x
, and
()
()
,1,2,,
!'()
k
k
f
ck
kf
α
α
==L
nn
ex
α
=−.
Consider the iteration function
()Fx
defined by
'( ) '( ( )) ( ( ))
() ()
'( ) 3 '( ( )) '( )
f
xfyx fzx
Fx zx
f
xfyxfx
+
=−
−+
(16)
Where
By some computations using Maple we can
obtain
()
( ) , ( ) 0, 1,2,3,4,5,6
i
FF i
αα α
===
(17)
(18)
Furthermore, from the Taylor expansion of
()
n
Fx
around
α
, we get
Substituting (18) into (19) yields
11
42 7 8
22 3
10 ( ) ( ).
nn
nn
xe
cc ce Oe
α
α
++
=+
=+ +
Therefore, we have
42 7 8
1223
10 ( ) ( )
nnn
eccceOe
+
=−+
which shows the seventh order of convergence.
To obtain an assessment of the efficiency of the
proposed method, we shall make use of efficiency
index, according to which the efficiency of an
iterative method is given by
1/
p
ω
, where
p
is the
order of the method and
ω
is the number of
function evaluations per iteration required by the
method. It is not hard to see that the efficiency
indices of the Algorithm 1 and Algorithm 2 are
1.431 and 1.476 respectively, which are better than
that of the classical Newton's method 1.414.
3 NUMERICAL RESULTS
Now, we employ Algorithm 1 and Algorithm 2 to
solve some nonlinear equations and compare them
with NM and the iterative method (PPM for short)
Potra and Pták presented in [7]
1
() ()
'( )
nn
nn
n
f
xfy
xx
fx
+
+
=−
(19)
which is cubically convergent with efficiency index
1.442, where
()
'( )
n
nn
n
f
x
yx
f
x
=−
.
Displayed in Table 1 are the number of iterations
(ITs) required such that
| ( ) | 1. 14.
n
fx E<−
In table 1, we use the following functions.
32
1
( ) 4 10, 1.36523001341410.fx x x
α
=+ =
2
( ) cos , 0.73908513321516.fx xx
α
=−=
3
3
() ( 1) 1, 2.fx x
α
=− =
2
730
4
() 1, 3.
xx
fx e
α
+−
=−=
22
5
( ) sin ( ) 1, 1.40449164885154.fx x x
α
=−+=
6
( ) ( 2) 1, 0.44285440096708.
x
fx x e
α
=+ =
7()
1
1
8
()
() () ( )
!
(( ) )
i
i
nn n
i
n
F
xFxF x
i
Ox
α
αα
α
+
=
==+
+−
2
2(()) (()) '(())
() () ,
'( )
'( )
()
() .
'( )
f
yx f yx f yx
zx yx
fx
fx
fx
yx x
fx
=− +
=−
(2) 4 (2) 2 (3)
(7)
6
525 ()[3 () 2'() ()]
() .
2'()
ffff
F
f
αααα
α
α
−+
=−
The computational results in Table 1 show that
Algorithm 1 requires less ITs than NM. Therefore,
Algorithm is of practical interest and can compete
with NM.
Table 1: Comparison of Algorithm 1, Algorithm 2, PPM
and NM
Func
-
tions
0
x
NM PPM
Algorithm
1
Algorith
m 2
1
f
1 5 3 3 3
1.46 4 3 3 3
2
f
0.5 4 3 3 3
3.12 7 4 3 3
3
f
2.5 6 3 3 3
1.45 7 5 4 4
4
f
4.2 16 8 6 6
3.4 12 5 4 4
5
f
1.8 5 4 3 3
2.1 5 4 4 3
6
f
7.6 12 9 5 5
-0.5 4 4 3 3
4 CONCLUSIONS
In order to obtain efficient iterative methods for the
nonlinear equations which come from the practical
problems in the materials science and manufacturing
technology field, in this paper, we present and
analyze two modified Newton-type iterative
methods for solving nonlinear equations. Both of the
algorithms are free from second derivatives. Several
numerical results illustrate the convergence behavior
and computational efficiency of the method
proposed in this paper. Computational results
demonstrate that they are more efficient and
performs better than the classical NM.
ACKNOWLEDGEMENTS
The work is supported by Project of Natural
Science Foundation of Shandong province
(ZR2016AM06), Excellent Young Scientist
Foundation of Shandong Province (BS2011SF024),
National Natural Science Foundation of China
(11601365).
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