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Vietnam Journal of Mechanics, VAST, Vol. 34, No. 4 (2012), pp. 321 – 325
Short Communication
DUAL APPROACH TO AVERAGED VALUES
OF FUNCTIONS:
ADVANCED FORMULAS
N. D. Anh
Institute of Mechanics, VAST, Vietnam
Abstract. Averaged values play major roles in the study of dynamic processes. The use
of those values allows transforming varying processes to some constant characteristics
that are much easier to be investigated. In order to extend the use of averaged values
one may apply the dual approach which suggests a consideration of two different aspects
of a problem in question. This short communication proposes new advanced formulas for
averaged values of functions based on the dual conception.
Key words: advanced formula, averaged value, global-local averaged, dual approach,
Duffing oscillator.
1. INTRODUCTION
Averaged values play major roles in the study of dynamic processes. The use of
those values allows transforming varying processes to some constant characteristics that
are much easier to be investigated. In order to extend the use of averaged values one may
apply the dual approach recently proposed and developed in [1]-[2]. One of significant
advantages of the dual conception is its consideration of two different aspects of a problem
in question which allows investigation to be more appropriate. This advantage has been
used in [3] to propose some new global and local averaged values of functions. The main
objective of the short communication is to present a further extension of global-local
averaged values of function. New advanced formulas for averaged values of functions are
proposed based on the dual conception.
2. ADVANCED FORMULAS FOR AVERAGED VALUES OF
DETERMINISTIC FUNCTIONS
Let y(x)be an integrable deterministic function of x∈[a, b]. The following advanced
formulas for averaged value of y(x)can be considered.
322 N. D. Anh
Classical formula. Define
I0(y(x), a, b) = y(x)(1)
Classical formula for averaged value of y(x)is well-known as follows
< y(x)>=< I 0(y(x), a, b)>=1
b−aZb
a
I0(y(x), a, b)dx =1
b−aZb
a
y(x)dx. (2)
Formula I.1. Define a function of x∈[a, b]by
I1(y(x), a, b) = 1
2(1
x−a
x
Z
a
y(σ)dσ +1
b−x
b
Z
x
y(σ)dσ).(3)
Formula I.1 for averaged value of y(x)is defined by
< y(x)>1=< I 1(y(x), a, b)>=1
b−aZb
a
I1(y(x), a, b)dx. (4)
Formula I.2. Define
I2(y(x), a, b) = I1(I1(y(x), a, b), a, b) =
=1
2(1
x−a
x
R
a
I1(y(σ), a, b)dσ +1
b−x
b
R
x
I1(y(σ), a, b)dσ).(5)
Formula I.2 for averaged value of y(x)is defined by
< y(x)>2=< I 2(y(x), a, b)) >=1
b−aZb
a
I2(y(x), a, b))dx. (6)
Analogously, one can define
In(y(x), a, b) = I1(In−1(y(x), a, b), a, b)(7)
and Formula I.n for averaged value of y(x)is defined by
< y(x)>n=< I n(y(x), a, b)>=1
b−aZb
a
In(y(x), a, b)dx. (8)
Further, according to (3) define
I1(y(r), a, x) = 1
2(1
r−a
r
Z
a
y(σ)dσ +1
x−r
x
Z
r
y(σ)dσ),
Dual approach to averaged values of functions: Advanced formulas 323
I1(y(s), x, b) = 1
2(1
s−x
s
Z
x
y(σ)dσ +1
b−s
b
Z
s
y(σ)dσ),(9)
and
A1(y(x), a, b) = 1
2(1
x−a
x
Z
a
I1(y(r), a, x)dr +1
b−x
b
Z
x
I1(y(s), x, b)ds).(10)
It is seen that I1(y(r), a, x)is a function of r∈[a, x],I1(y(s), x, b)is a function of s∈[x, b],
and A1(y(x), a, b)is a function of x∈[a, b].Formula A.1 for averaged value of function
y(x)is defined by
< y(x)>1=< A1(y(x), a, b)>=1
b−aZb
a
A1(y(x), a, b)dx, (11)
Analogously, one can define
An(y(x), a, b) = A1(An−1(y(x), a, b), a, b)(12)
and Formula A.n for averaged value of y(x)is defined by
< y(x)>n=< An(y(x), a, b)>=1
b−aZb
a
An(y(x), a, b)dx. (13)
One can also define mixed products as
An(Im(y(x), a, b), a, b) = A1(An−1(Im(y(x), a, b), a, b), a, b)(14)
and Formula A.nI.m for averaged value of y(x)as
< y(x)>n
m=< An(Im(y(x), a, b), a, b)>=1
b−aZb
a
An(Im(y(x), a, b), a, b)dx. (15)
3. APPLICATION TO NONLINEAR EQUATIONS
For illustration of possible uses of the proposed advanced formulas consider the
following equation
¨z+γz3= 0, z(0) = a, ˙z(0) = 0.(16)
Let xis a solution of the linear equation
¨x+kx = 0, x(0) = a, ˙x(0) = 0.(17)
324 N. D. Anh
The equation error is to be
e(x) = γx3−kx
The value of kcan be determined from a minimum condition, for example,
L(e2(x)) →min
k(18)
where Lis a linear averaging operator. Thus, from (18) one has
ω2=k=γLx4
L(x2)(19)
- Taking
L(·) = 1
aZa
0
(·)dx (20)
one gets
ω2
0=k0=γ
1
aRa
0x4dx
1
aRa
0x2dx
=γa4
5
3
a2=3
5γa2,(21)
or,
ω0=r3
5γa2= 0.77460√γa. (22)
- Taking
L(·) = <·>1=1
aZa
0
I1(·,0, a )dx, (23)
one gets
ω2
1=k1=γ< x4>1
< x2>1
=γ
1
aRa
0
1
10(a4+a3x+a2x2+ax3+ 2x4)dx
1
aRa
0
1
6(a2+ax + 2x2)dx
=
=γ149a4
600
36
13a2=447
650γa2,
or,
ω1=r447
650γa2= 0.82927√γa. (24)
- Taking
L(·) = <·>2=1
aZa
0
I2(·,0, a )dx, (25)
Dual approach to averaged values of functions: Advanced formulas 325
one gets
ω2
2=k2=γ< x4>2
< x2>2
=γ
1
aRa
0
1
1200(209a4+ 119a3x+ 79a2x2+ 54ax3+ 48x4)dx
1
aRa
0
1
72(19a2+ 10ax + 8x2)dx
=
= 0.2649427
10γ a2= 0.71535γa2,
(26)
or,
ω2=p0.71535γa2= 0.84578√γa. (27)
Comparing the solution (27) with the exact solution ωeand the one ωlobtained by the
classical criterion of equivalent linearization, respectively,
ωe= 0.847√γa, ωl= 0.866√γa, (28)
one shows a significant accuracy of (27).
4. CONCLUSION
In this short communication the main idea of the dual conception is further extended
to suggest new advanced formulas for averaged values of functions. These advanced for-
mulas contain the classical formula of averaged value as a particular case. In the example
of Duffing oscillator it is shown that advanced formulas can give a series of approximate
solutions that are more accurate than the conventional one obtained by the classical cri-
terion of equivalent linearization.
ACKNOWLEDGEMENTS
The research reported in this paper is supported by Vietnam National Foundation
for Science and Technology Development.
REFERENCES
[1] N. D. Anh, Duality in the analysis of responses to nonlinear systems, Vietnam Journal of
Mechanics,32(4) (2010) 263-266.
[2] N. D. Anh, N. N. Hieu, N. N. Linh, A dual criterion of equivalent linearization method for non-
linear systems subjected to random excitation, Acta Mechanica, (2012) DOI 10.1007/s00707-
011-0582-z.
[3] N. D. Anh, Dual approach to averaged values of functions, Vietnam Journal of Mechanics,
34(3) (2012) 211-214.
Received April 16, 2012