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Research ArticleLocal Fractional Variational Iteration andDecomposition Methods for Wave Equation onCantor Sets within Local Fractional Operators
Dumitru Baleanu123 J A Tenreiro Machado4 Carlo Cattani5
Mihaela Cristina Baleanu6 and Xiao-Jun Yang7
1 Department of Chemical and Materials Engineering Faculty of Engineering King Abdulaziz UniversityPO Box 80204 Jeddah 21589 Saudi Arabia
2Department of Mathematics and Computer Sciences Faculty of Arts and Sciences Cankaya University06530 Ankara Turkey
3 Institute of Space Sciences Magurele Bucharest Romania4Department of Electrical Engineering Institute of Engineering Polytechnic of Porto Rua Dr AntonioBernardino de Almeida 431 4200-072 Porto Portugal
5 Department of Mathematics University of Salerno Via Ponte don Melillo Fisciano 84084 Salerno Italy6Mihail SadoveanuTheoretical High School District 2 Street Popa Lazar No 8 021586 Bucharest Romania7Department of Mathematics and Mechanics China University of Mining and Technology Xuzhou CampusXuzhou Jiangsu 221008 China
Correspondence should be addressed to Xiao-Jun Yang dyangxiaojun163com
Received 9 November 2013 Accepted 8 December 2013 Published 2 January 2014
Academic Editor Ming Li
Copyright copy 2014 Dumitru Baleanu et al This is an open access article distributed under the Creative Commons AttributionLicense which permits unrestricted use distribution and reproduction in any medium provided the original work is properlycited
We perform a comparison between the fractional iteration and decomposition methods applied to the wave equation on Cantorset The operators are taken in the local sense The results illustrate the significant features of the two methods which are both veryeffective and straightforward for solving the differential equations with local fractional derivative
1 Introduction
Many problems of physics and engineering are expressed byordinary and partial differential equations which are termedboundary value problems We can mention for examplethe wave the Laplace the Klein-Gordon the Schrodingerrsquosthe telegraph the Advection the Burgers the KdV theBoussinesq and the Fisher equations and others [1]
Recently the fractional calculus theory was recognized tobe a good tool for modeling complex problems demonstrat-ing its applicability in numerical scientific disciplines Bound-ary value problems for the fractional differential equationshave been the focus of several studies due to their frequentappearance in various areas such as fractional diffusion
and wave [2] fractional telegraph [3] fractional KdV [4]fractional Schrodinger [5] fractional evolution [6] fractionalNavier-Stokes [7] fractionalHeisenberg [8] fractional Klein-Gordon [9] and fractional Fisher equations [10]
Several analytical and numerical techniques were suc-cessfully applied to deal with differential equations frac-tional differential equations and local fractional differentialequations (see eg [1ndash36] and the references therein) Thetechniques include the heat-balance integral [11] the frac-tional Fourier [12] the fractional Laplace transform [12] theharmonic wavelet [13 14] the local fractional Fourier andLaplace transform [15] local fractional variational iteration[16 17] the local fractional decomposition [18] and thegeneralized local fractional Fourier transform [19] methods
Hindawi Publishing CorporationAbstract and Applied AnalysisVolume 2014 Article ID 535048 6 pageshttpdxdoiorg1011552014535048
2 Abstract and Applied Analysis
Recently the wave equation on Cantor sets (local frac-tional wave equation) was given by [35]
1205972120572119906 (119909 119905)
1205971199052120572minus 1198862120572 1205972120572119906 (119909 119905)
1205971199092120572= 0 (1)
where the operators are local fractional ones [16ndash19 35 36]Following (1) a wave equation on Cantor sets was
proposed as follows [36]
1205972120572119906 (119909 119905)
1205971199052120572minus
1199092120572
Γ (1 + 2120572)
1205972120572119906 (119909 119905)
1205971199092120572= 0 (2)
where 119906(119909 119905) is a fractal wave functionIn this paper our purpose is to compare the local
fractional variational iteration and decomposition methodsfor solving the local fractional differential equations Forillustrating the concepts we adopt one example for solving thewave equation on Cantor sets with local fractional operator
Bearing these ideas in mind the paper is organized asfollows In Section 2 we present basic definitions and providesome properties of local fractional derivative and integrationIn Section 3 we introduce the local fractional variationaliteration and the decomposition methods In Section 4 wediscuss one application Finally in Section 5 we outline themain conclusions
2 Mathematical Tools
We recall in this section the notations and some properties ofthe local fractional operators [15ndash19 35 36]
Definition 1 (see [15ndash19 35 36]) The function 119891(119909) is localfractional continuous if it is valid for
1003816100381610038161003816119891 (119909) minus 119891 (1199090)1003816100381610038161003816 lt 120576120572 (3)
where |119909 minus 1199090| lt 120575 for 120576 gt 0 and 120576 isin 119877
We notice that there are existence conditions of localfractional continuities that operating functions are right-hand and left-hand local fractional continuity Meanwhilethe right-hand local fractional continuity is equal to its left-hand local fractional continuity For more details see [35]
Following (4) we have [15ndash19 35 36]
1205881205721003816100381610038161003816119909 minus 119909
0
1003816100381610038161003816120572
le1003816100381610038161003816119891 (119909) minus 119891 (119909
0)1003816100381610038161003816 le 1205811205721003816100381610038161003816119909 minus 119909
0
1003816100381610038161003816120572 (4)
with |119909 minus 1199090| lt 120575 for 120576 120575 gt 0 and 120576 120575 120581 120588 isin 119877
For a fractal set 119865 there is a fractal measure [35]
119867120572(119865 cap (119909 119909
0)) = (119909 minus 119909
0)120572
(5)
where 119891(119909) presents a bi-Lipschitz mapping with fractaldimension 120572 and119867
120572 denotes a Hausdorff dimensionWe verify that there is a measure
1198671(119865 cap (119909 119909
0)) = 119909 minus 119909
0(6)
in the case of 120572 = 1 and 119891(119909) is a Lipschitz mapping If 119865 isa Cantor set we have 119867ln 2 ln 3
(119865 cap (119909 1199090)) = (119909 minus 119909
0)ln 2 ln 3
with 120572 = ln 2 ln 3
Definition 2 (see [15ndash19 35 36]) The local fractional deriva-tive of 119891(119909) at 119909 = 119909
0is defined as [16ndash20]
119891(120572)
(1199090) =
119889120572119891 (119909)
119889119909120572
10038161003816100381610038161003816100381610038161003816119909=1199090
= lim119909rarr1199090
Δ120572(119891 (119909) minus 119891 (119909
0))
(119909 minus 1199090)120572
(7)
where
Δ120572(119891 (119909) minus 119891 (119909
0)) cong Γ (1 + 120572) Δ (119891 (119909) minus 119891 (119909
0)) (8)
We find that the existence condition for local fractionalderivative of 119891(119909) is that the right-hand local fractionalderivative is equal to the left-hand local fractional derivative(see eg [16 35] and the references therein)
Definition 3 (see [15ndash19 35 36]) A partition of the interval[119886 119887] is denoted as (119905
119895 119905119895+1
) 119895 = 0 119873 minus 1 1199050= 119886 and
119905119873
= 119887 with Δ119905119895= 119905119895+1
minus 119905119895and Δ119905 = maxΔ119905
0 Δ1199051 Δ119905119895
Local fractional integral of 119891(119909) in the interval [119886 119887] is givenby
119886119868119887
(120572)119891 (119909) =
1
Γ (1 + 120572)int
119887
119886
119891 (119905) (119889119905)120572
=1
Γ (1 + 120572)limΔ119905rarr0
119895=119873minus1
sum
119895=0
119891 (119905119895) (Δ119905119895)120572
(9)
If the functions are local fractional continuous then thelocal fractional derivatives and integrals exist That is tosay operating functions have nondifferentiable and fractalproperties (see [35] and the references therein)
Some properties of local fractional derivative and inte-grals are given in [35]
3 Analytical Methods
In order to illustrate two analytical methods we investigatethe nonlinear local fractional equation as follows
119871(119899)
120572119906 + 119877120572119906 = 0 (10)
where 119871(119899)
120572is linear local fractional operators respectively
with 119899 = 1 2 and 119877120572is linear local fractional operators of
order less than 119871(119899)
120572
31 Local Fractional Variational Iteration Method The localfractional variational iteration algorithm is given by [16 17]on the line of the formalism suggested in [35]
119906119899+1
(119905) = 119906119899(119905) +
1
Γ (1 + 120572)
times int
119905
0
120582120572
Γ (1 + 120572)119871(119899)
120572119906119899(119904) + 119877
120572119906119899(119904) (119889119904)
120572
(11)
Here we can construct a correction functional as follows [1617]
119906119899+1
(119905) = 119906119899(119905) +
1
Γ (1 + 120572)
times int
119905
0
120582120572
Γ (1 + 120572)119871(119899)
120572119906119899(119904) + 119877
120572119899(119904) (119889119904)
120572
(12)
Abstract and Applied Analysis 3
where 119899is considered as a restricted local fractional varia-
tion that is 120575120572119899= 0 (for more details see [35])
For 119899 = 2 we have
120582120572=
(119904 minus 119905)120572
Γ (1 + 120572) (13)
so that iteration is expressed as
119906119899+1
(119905) = 119906119899(119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)119871(119899)
120572119906119899(119904) + 119877
120572119906119899(119904) (119889119904)
120572
(14)
Finally the solution is
119906 (119909) = lim119899rarrinfin
119906119899(119909) (15)
32 Local Fractional Decomposition Method When 119871(119899)
120572in
(10) is a local fractional differential operator of order 2120572 wedenote it as
119871(119899)
120572= 119871(2120572)
119909119909=
1205972120572
1205971199092120572
119877120572119906 (119905) =
120597120572
120597119909120572119906 (119905) + 119891 (119905)
(16)
By defining the 119899-fold local fractional integral operator
119871(minus2)
120572119898(119904) =
0119868119909(120572)
0119868119909(120572)
119898(119904) (17)
we get
119871(minus2)
120572119871(2)
120572119906 (119904) = 119871
(minus2)
120572119877120572119906 (119904) (18)
Thus
119906 (119904) = 119903 (119909) + 119871(minus2)
120572119877120572119906 (119904) (19)
where the term 119903(119909) is to be determined from the fractalinitial conditions
Therefore we get the iterative formula as follows
119906 (119909) = 1199060(119909) + 119871
(minus2)
120572119877120572119906 (119904) (20)
with 1199060(119909) = 119903(119909)
Hence for 119899 ge 0 we have the following recurrencerelationship
119906119899+1
(119909) = 119871(minus2)
120572119877120572119906119899(119904)
1199060(119909) = 119903 (119909)
(21)
Finally the solution can be constructed as
119906 (119909) = lim119899rarrinfin
120601119899(119909) = lim
119899rarrinfin
infin
sum
119899=0
119906119899(119909) (22)
For more details see [18]
4 An Illustrative Example
In this section one example for wave equation is presented inorder to demonstrate the simplicity and the efficiency of theabove methods
In (2) we consider the following initial and boundaryconditions
120597120572119906 (119909 0)
120597119905120572= 0 119906 (119909 0) =
1199092120572
Γ (1 + 2120572) (23)
Using (14) we have the iterative formula
119906119899+1
(119909 119905)
= 119906119899(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1205972120572119906119899(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
1205972120572119906119899(119909 119904)
1205971199092120572(119889119904)120572
(24)
where the initial value is given by
1199060(119909 119905) =
1199092120572
Γ (1 + 2120572) (25)
Thus after computing (23) we obtain
1199061(119909 119905)
= 1199060(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199060(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
12059721205721199060(119909 119904)
1205971199092120572(119889119904)120572
= 1199060(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)(1 +
1199052120572
Γ (1 + 2120572))
1199062(119909 119905)
= 1199061(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199061(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
12059721205721199061(119909 119904)
1205971199092120572(119889119904)120572
= 1199061(119909 119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572)
1199042120572
Γ (1 + 2120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)(1 +
1199052120572
Γ (1 + 2120572)+
1199054120572
Γ (1 + 4120572))
4 Abstract and Applied Analysis
1199063(119909 119905)
= 1199062(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199062(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
12059721205721199062(119909 119904)
1205971199092120572(119889119904)120572
= 1199062(119909 119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572)
1199054120572
Γ (1 + 4120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)
3
sum
119894=0
1199052119894120572
Γ (1 + 2119894120572)
1199064(119909 119905)
= 1199063(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199063(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
1199092120572
Γ (1 + 2120572)
12059721205721199063(119909 119904)
1205971199092120572(119889119904)120572
= 1199063(119909 119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572)
1199056120572
Γ (1 + 6120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)
4
sum
119894=0
1199052119894120572
Γ (1 + 2119894120572)
(26)
119906119899(119909 119905)
= 119906119899minus1
(119909 119905) +1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1205972120572119906119899minus1
(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
1205972120572119906119899minus1
(119909 119904)
1205971199092120572(119889119904)120572
=1199092120572
Γ (1 + 2120572)
119899
sum
119894=0
1199052119894120572
Γ (1 + 2119894120572)
(27)
Hence from (27) we obtain the solution of (3) as
119906 (119909) = lim119899rarrinfin
119906119899(119909) =
1199092120572
Γ (1 + 2120572)cosh120572(119905120572) (28)
Here from (21) we get
119906119899+1
(119909 119905) =0119868119905(120572)
0119868119905(120572) 119909
2120572
Γ (1 + 2120572)
1205972120572119906119899(119909 119904)
1205971199092120572
1199060(119909 119905) =
1199092120572
Γ (1 + 2120572)
(29)
Therefore from (29) we give the components as follows
1199060(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199061(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199052120572
Γ (1 + 2120572)
1199062(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199054120572
Γ (1 + 4120572)
1199063(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199053120572
Γ (1 + 6120572)
1199064(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199058120572
Γ (1 + 8120572)
119906119899(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199052119899120572
Γ (1 + 2119899120572)
(30)
Consequently the exact solution is given by
119906 (119909 119905) = lim119899rarrinfin
infin
sum
119899=0
119906119899(119909 119905)
= lim119899rarrinfin
infin
sum
119899=0
1199092120572
Γ (1 + 2120572)
1199052119899120572
Γ (1 + 2119899120572)
=1199092120572
Γ (1 + 2120572)cosh120572(119909120572)
(31)
where
cosh120572(119909120572) =
infin
sum
119899=0
1199052119899120572
Γ (1 + 2119899120572) (32)
The solution of (2) for 120572 = ln 2 ln 3 is depicted in Figure 1
5 Conclusions
In this work we developed a comparison between thevariational iteration method and the decomposition methodwithin local fractional operators The two approaches con-stitute efficient tools to handle the approximation solutionsfor differential equations on Cantor sets with local fractionalderivative We notice that the fractional variational iterationmethod gives the several successive approximate formulasusing the iteration of the correction local fractional func-tional However the local fractional decomposition method
Abstract and Applied Analysis 5
25
2
15
1
05
01
05
0 002
0406
081
x
t
u(xt)
Figure 1 Graph of 119906(119909 119905) for 120572 = ln 2 ln 3
provides the components of the exact solution which is localfractional continuous function where these componentsare also local fractional continuous functions Both thevariational iteration method and the decomposition methodwithin local fractional operators provide the solution insuccessive componentsThemethods are structured to get thelocal fractional series solution which is a nondifferentiablefunction
Conflict of Interests
The authors declare that there is no conflict of interestsregarding publication of this paper
References
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[2] W R Schneider and W Wyss ldquoFractional diffusion and waveequationsrdquo Journal of Mathematical Physics vol 30 no 1 pp134ndash144 1989
[3] Z G Zhao and C P Li ldquoFractional differencefinite elementapproximations for the time-space fractional telegraph equa-tionrdquo Applied Mathematics and Computation vol 219 no 6 pp2975ndash2988 2012
[4] S Momani Z Odibat and A Alawneh ldquoVariational iterationmethod for solving the space- and time-fractional KdV equa-tionrdquo Numerical Methods for Partial Differential Equations vol24 no 1 pp 262ndash271 2008
[5] N Laskin ldquoFractional Schrodinger equationrdquo Physical ReviewE vol 66 Article ID 056108 2002
[6] Y Zhou and F Jiao ldquoNonlocal Cauchy problem for fractionalevolution equationsrdquo Nonlinear Analysis Real World Applica-tions vol 11 no 5 pp 4465ndash4475 2010
[7] S Momani and Z Odibat ldquoAnalytical solution of a time-fractional Navier-Stokes equation by Adomian decompositionmethodrdquo Applied Mathematics and Computation vol 177 no 2pp 488ndash494 2006
[8] V E Tarasov ldquoFractional Heisenberg equationrdquo Physics LettersA vol 372 no 17 pp 2984ndash2988 2008
[9] A K Golmankhaneh A K Golmankhaneh and D BaleanuldquoOn nonlinear fractional KleinGordon equationrdquo Signal Pro-cessing vol 91 no 3 pp 446ndash451 2011
[10] Z B Li W H Zhu and L L Huang ldquoApplication of fractionalvariational iteration method to time-fractional Fisher equa-tionrdquo Advanced Science Letters vol 10 no 1 pp 610ndash614 2012
[11] J Hristov ldquoHeat-balance integral to fractional (half-time) heatdiffusion sub-modelrdquoThermal Science vol 14 no 2 pp 291ndash3162010
[12] D Baleanu K Diethelm E Scalas and J J Trujillo FractionalCalculus Models and Numerical Methods vol 3 of Series onComplexity Nonlinearity and Chaos World Scientific BostonMass USA 2012
[13] C Cattani ldquoHarmonic wavelet solution of Poissonrsquos problemrdquoBalkan Journal of Geometry and Its Applications vol 13 no 1pp 27ndash37 2008
[14] C Cattani ldquoHarmonic wavelets towards the solution of nonlin-ear PDErdquo Computers amp Mathematics with Applications vol 50no 8-9 pp 1191ndash1210 2005
[15] X J Yang Local Fractional Functional Analysis and Its Applica-tions Asian Academic Hong Kong China 2011
[16] X J Yang and D Baleanu ldquoFractal heat conduction problemsolved by local fractional variation iteration methodrdquo ThermalScience vol 17 no 2 pp 625ndash628 2013
[17] W-H Su D Baleanu X-J Yang and H Jafari ldquoDamped waveequation and dissipative wave equation in fractal strings withinthe local fractional variational iteration methodrdquo Fixed PointTheory and Applications vol 2013 article 89 2013
[18] X J Yang D Baleanu and W P Zhong ldquoApproximation solu-tions for diffusion equation on Cantor time-spacerdquo Proceedingof the Romanian Academy A vol 14 no 2 pp 127ndash133 2013
[19] X J Yang D Baleanu and J A T Machado ldquoMathematicalaspects of Heisenberg uncertainty principle within local frac-tional Fourier analysisrdquoBoundary Value Problems no 1 pp 131ndash146 2013
[20] J Klafter S C Lim and RMetzler Fractional Dynamics RecentAdvances World Scientific Singapore 2012
[21] J Sabatier O P Agrawal and J T Machado Advances inFractional Calculus Theoretical Developments and Applicationsin Physics and Engineering Springer 2007
[22] R Hilfer Applications of Fractional Calculus in Physics WordScientific Singapore 2000
[23] M Li S C Lim and S Chen ldquoExact solution of impulseresponse to a class of fractional oscillators and its stabilityrdquoMathematical Problems in Engineering vol 2011 Article ID657839 9 pages 2011
[24] K M Kolwankar and A D Gangal ldquoLocal fractional Fokker-Planck equationrdquo Physical Review Letters vol 80 no 2 pp 214ndash217 1998
[25] K M Kolwankar and A D Gangal ldquoFractional differentiabilityof nowhere differentiable functions and dimensionsrdquo Chaosvol 6 no 4 pp 505ndash513 1996
[26] A Babakhani and V Daftardar-Gejji ldquoOn calculus of localfractional derivativesrdquo Journal of Mathematical Analysis andApplications vol 270 no 1 pp 66ndash79 2002
[27] Y Chen Y Yan and K Zhang ldquoOn the local fractionalderivativerdquo Journal of Mathematical Analysis and Applicationsvol 362 no 1 pp 17ndash33 2010
[28] A Carpinteri B Chiaia and P Cornetti ldquoStatic-kinematicduality and the principle of virtual work in the mechanics of
6 Abstract and Applied Analysis
fractal mediardquo Computer Methods in Applied Mechanics andEngineering vol 191 no 1-2 pp 3ndash19 2001
[29] A Carpinteri B Chiaia and P Cornetti ldquoThe elastic problemfor fractal media basic theory and finite element formulationrdquoComputers and Structures vol 82 no 6 pp 499ndash508 2004
[30] A Carpinteri and P Cornetti ldquoA fractional calculus approach tothe description of stress and strain localization in fractalmediardquoChaos Solitons amp Fractals vol 13 no 1 pp 85ndash94 2002
[31] F Ben Adda and J Cresson ldquoAbout non-differentiable func-tionsrdquo Journal of Mathematical Analysis and Applications vol263 no 2 pp 721ndash737 2001
[32] W Chen ldquoTime-space fabric underlying anomalous diffusionrdquoChaos Solitons amp Fractals vol 28 no 4 pp 923ndash929 2006
[33] W Chen H G Sun X D Zhang and D Korosak ldquoAnoma-lous diffusion modeling by fractal and fractional derivativesrdquoComputers amp Mathematics with Applications vol 59 no 5 pp1754ndash1758 2010
[34] G Jumarie ldquoModified Riemann-Liouville derivative and frac-tional Taylor series of nondifferentiable functions furtherresultsrdquoComputersampMathematics with Applications vol 51 no9-10 pp 1367ndash1376 2006
[35] X J Yang Advanced Local Fractional Calculus and Its Applica-tions World Science New York NY USA 2012
[36] A-M Yang X-J Yang and Z-B Li ldquoLocal fractional seriesexpansion method for solving wave and diffusion equations onCantor setsrdquoAbstract and Applied Analysis vol 2013 Article ID351057 5 pages 2013
Submit your manuscripts athttpwwwhindawicom
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Stochastic AnalysisInternational Journal of
2 Abstract and Applied Analysis
Recently the wave equation on Cantor sets (local frac-tional wave equation) was given by [35]
1205972120572119906 (119909 119905)
1205971199052120572minus 1198862120572 1205972120572119906 (119909 119905)
1205971199092120572= 0 (1)
where the operators are local fractional ones [16ndash19 35 36]Following (1) a wave equation on Cantor sets was
proposed as follows [36]
1205972120572119906 (119909 119905)
1205971199052120572minus
1199092120572
Γ (1 + 2120572)
1205972120572119906 (119909 119905)
1205971199092120572= 0 (2)
where 119906(119909 119905) is a fractal wave functionIn this paper our purpose is to compare the local
fractional variational iteration and decomposition methodsfor solving the local fractional differential equations Forillustrating the concepts we adopt one example for solving thewave equation on Cantor sets with local fractional operator
Bearing these ideas in mind the paper is organized asfollows In Section 2 we present basic definitions and providesome properties of local fractional derivative and integrationIn Section 3 we introduce the local fractional variationaliteration and the decomposition methods In Section 4 wediscuss one application Finally in Section 5 we outline themain conclusions
2 Mathematical Tools
We recall in this section the notations and some properties ofthe local fractional operators [15ndash19 35 36]
Definition 1 (see [15ndash19 35 36]) The function 119891(119909) is localfractional continuous if it is valid for
1003816100381610038161003816119891 (119909) minus 119891 (1199090)1003816100381610038161003816 lt 120576120572 (3)
where |119909 minus 1199090| lt 120575 for 120576 gt 0 and 120576 isin 119877
We notice that there are existence conditions of localfractional continuities that operating functions are right-hand and left-hand local fractional continuity Meanwhilethe right-hand local fractional continuity is equal to its left-hand local fractional continuity For more details see [35]
Following (4) we have [15ndash19 35 36]
1205881205721003816100381610038161003816119909 minus 119909
0
1003816100381610038161003816120572
le1003816100381610038161003816119891 (119909) minus 119891 (119909
0)1003816100381610038161003816 le 1205811205721003816100381610038161003816119909 minus 119909
0
1003816100381610038161003816120572 (4)
with |119909 minus 1199090| lt 120575 for 120576 120575 gt 0 and 120576 120575 120581 120588 isin 119877
For a fractal set 119865 there is a fractal measure [35]
119867120572(119865 cap (119909 119909
0)) = (119909 minus 119909
0)120572
(5)
where 119891(119909) presents a bi-Lipschitz mapping with fractaldimension 120572 and119867
120572 denotes a Hausdorff dimensionWe verify that there is a measure
1198671(119865 cap (119909 119909
0)) = 119909 minus 119909
0(6)
in the case of 120572 = 1 and 119891(119909) is a Lipschitz mapping If 119865 isa Cantor set we have 119867ln 2 ln 3
(119865 cap (119909 1199090)) = (119909 minus 119909
0)ln 2 ln 3
with 120572 = ln 2 ln 3
Definition 2 (see [15ndash19 35 36]) The local fractional deriva-tive of 119891(119909) at 119909 = 119909
0is defined as [16ndash20]
119891(120572)
(1199090) =
119889120572119891 (119909)
119889119909120572
10038161003816100381610038161003816100381610038161003816119909=1199090
= lim119909rarr1199090
Δ120572(119891 (119909) minus 119891 (119909
0))
(119909 minus 1199090)120572
(7)
where
Δ120572(119891 (119909) minus 119891 (119909
0)) cong Γ (1 + 120572) Δ (119891 (119909) minus 119891 (119909
0)) (8)
We find that the existence condition for local fractionalderivative of 119891(119909) is that the right-hand local fractionalderivative is equal to the left-hand local fractional derivative(see eg [16 35] and the references therein)
Definition 3 (see [15ndash19 35 36]) A partition of the interval[119886 119887] is denoted as (119905
119895 119905119895+1
) 119895 = 0 119873 minus 1 1199050= 119886 and
119905119873
= 119887 with Δ119905119895= 119905119895+1
minus 119905119895and Δ119905 = maxΔ119905
0 Δ1199051 Δ119905119895
Local fractional integral of 119891(119909) in the interval [119886 119887] is givenby
119886119868119887
(120572)119891 (119909) =
1
Γ (1 + 120572)int
119887
119886
119891 (119905) (119889119905)120572
=1
Γ (1 + 120572)limΔ119905rarr0
119895=119873minus1
sum
119895=0
119891 (119905119895) (Δ119905119895)120572
(9)
If the functions are local fractional continuous then thelocal fractional derivatives and integrals exist That is tosay operating functions have nondifferentiable and fractalproperties (see [35] and the references therein)
Some properties of local fractional derivative and inte-grals are given in [35]
3 Analytical Methods
In order to illustrate two analytical methods we investigatethe nonlinear local fractional equation as follows
119871(119899)
120572119906 + 119877120572119906 = 0 (10)
where 119871(119899)
120572is linear local fractional operators respectively
with 119899 = 1 2 and 119877120572is linear local fractional operators of
order less than 119871(119899)
120572
31 Local Fractional Variational Iteration Method The localfractional variational iteration algorithm is given by [16 17]on the line of the formalism suggested in [35]
119906119899+1
(119905) = 119906119899(119905) +
1
Γ (1 + 120572)
times int
119905
0
120582120572
Γ (1 + 120572)119871(119899)
120572119906119899(119904) + 119877
120572119906119899(119904) (119889119904)
120572
(11)
Here we can construct a correction functional as follows [1617]
119906119899+1
(119905) = 119906119899(119905) +
1
Γ (1 + 120572)
times int
119905
0
120582120572
Γ (1 + 120572)119871(119899)
120572119906119899(119904) + 119877
120572119899(119904) (119889119904)
120572
(12)
Abstract and Applied Analysis 3
where 119899is considered as a restricted local fractional varia-
tion that is 120575120572119899= 0 (for more details see [35])
For 119899 = 2 we have
120582120572=
(119904 minus 119905)120572
Γ (1 + 120572) (13)
so that iteration is expressed as
119906119899+1
(119905) = 119906119899(119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)119871(119899)
120572119906119899(119904) + 119877
120572119906119899(119904) (119889119904)
120572
(14)
Finally the solution is
119906 (119909) = lim119899rarrinfin
119906119899(119909) (15)
32 Local Fractional Decomposition Method When 119871(119899)
120572in
(10) is a local fractional differential operator of order 2120572 wedenote it as
119871(119899)
120572= 119871(2120572)
119909119909=
1205972120572
1205971199092120572
119877120572119906 (119905) =
120597120572
120597119909120572119906 (119905) + 119891 (119905)
(16)
By defining the 119899-fold local fractional integral operator
119871(minus2)
120572119898(119904) =
0119868119909(120572)
0119868119909(120572)
119898(119904) (17)
we get
119871(minus2)
120572119871(2)
120572119906 (119904) = 119871
(minus2)
120572119877120572119906 (119904) (18)
Thus
119906 (119904) = 119903 (119909) + 119871(minus2)
120572119877120572119906 (119904) (19)
where the term 119903(119909) is to be determined from the fractalinitial conditions
Therefore we get the iterative formula as follows
119906 (119909) = 1199060(119909) + 119871
(minus2)
120572119877120572119906 (119904) (20)
with 1199060(119909) = 119903(119909)
Hence for 119899 ge 0 we have the following recurrencerelationship
119906119899+1
(119909) = 119871(minus2)
120572119877120572119906119899(119904)
1199060(119909) = 119903 (119909)
(21)
Finally the solution can be constructed as
119906 (119909) = lim119899rarrinfin
120601119899(119909) = lim
119899rarrinfin
infin
sum
119899=0
119906119899(119909) (22)
For more details see [18]
4 An Illustrative Example
In this section one example for wave equation is presented inorder to demonstrate the simplicity and the efficiency of theabove methods
In (2) we consider the following initial and boundaryconditions
120597120572119906 (119909 0)
120597119905120572= 0 119906 (119909 0) =
1199092120572
Γ (1 + 2120572) (23)
Using (14) we have the iterative formula
119906119899+1
(119909 119905)
= 119906119899(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1205972120572119906119899(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
1205972120572119906119899(119909 119904)
1205971199092120572(119889119904)120572
(24)
where the initial value is given by
1199060(119909 119905) =
1199092120572
Γ (1 + 2120572) (25)
Thus after computing (23) we obtain
1199061(119909 119905)
= 1199060(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199060(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
12059721205721199060(119909 119904)
1205971199092120572(119889119904)120572
= 1199060(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)(1 +
1199052120572
Γ (1 + 2120572))
1199062(119909 119905)
= 1199061(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199061(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
12059721205721199061(119909 119904)
1205971199092120572(119889119904)120572
= 1199061(119909 119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572)
1199042120572
Γ (1 + 2120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)(1 +
1199052120572
Γ (1 + 2120572)+
1199054120572
Γ (1 + 4120572))
4 Abstract and Applied Analysis
1199063(119909 119905)
= 1199062(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199062(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
12059721205721199062(119909 119904)
1205971199092120572(119889119904)120572
= 1199062(119909 119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572)
1199054120572
Γ (1 + 4120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)
3
sum
119894=0
1199052119894120572
Γ (1 + 2119894120572)
1199064(119909 119905)
= 1199063(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199063(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
1199092120572
Γ (1 + 2120572)
12059721205721199063(119909 119904)
1205971199092120572(119889119904)120572
= 1199063(119909 119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572)
1199056120572
Γ (1 + 6120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)
4
sum
119894=0
1199052119894120572
Γ (1 + 2119894120572)
(26)
119906119899(119909 119905)
= 119906119899minus1
(119909 119905) +1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1205972120572119906119899minus1
(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
1205972120572119906119899minus1
(119909 119904)
1205971199092120572(119889119904)120572
=1199092120572
Γ (1 + 2120572)
119899
sum
119894=0
1199052119894120572
Γ (1 + 2119894120572)
(27)
Hence from (27) we obtain the solution of (3) as
119906 (119909) = lim119899rarrinfin
119906119899(119909) =
1199092120572
Γ (1 + 2120572)cosh120572(119905120572) (28)
Here from (21) we get
119906119899+1
(119909 119905) =0119868119905(120572)
0119868119905(120572) 119909
2120572
Γ (1 + 2120572)
1205972120572119906119899(119909 119904)
1205971199092120572
1199060(119909 119905) =
1199092120572
Γ (1 + 2120572)
(29)
Therefore from (29) we give the components as follows
1199060(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199061(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199052120572
Γ (1 + 2120572)
1199062(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199054120572
Γ (1 + 4120572)
1199063(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199053120572
Γ (1 + 6120572)
1199064(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199058120572
Γ (1 + 8120572)
119906119899(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199052119899120572
Γ (1 + 2119899120572)
(30)
Consequently the exact solution is given by
119906 (119909 119905) = lim119899rarrinfin
infin
sum
119899=0
119906119899(119909 119905)
= lim119899rarrinfin
infin
sum
119899=0
1199092120572
Γ (1 + 2120572)
1199052119899120572
Γ (1 + 2119899120572)
=1199092120572
Γ (1 + 2120572)cosh120572(119909120572)
(31)
where
cosh120572(119909120572) =
infin
sum
119899=0
1199052119899120572
Γ (1 + 2119899120572) (32)
The solution of (2) for 120572 = ln 2 ln 3 is depicted in Figure 1
5 Conclusions
In this work we developed a comparison between thevariational iteration method and the decomposition methodwithin local fractional operators The two approaches con-stitute efficient tools to handle the approximation solutionsfor differential equations on Cantor sets with local fractionalderivative We notice that the fractional variational iterationmethod gives the several successive approximate formulasusing the iteration of the correction local fractional func-tional However the local fractional decomposition method
Abstract and Applied Analysis 5
25
2
15
1
05
01
05
0 002
0406
081
x
t
u(xt)
Figure 1 Graph of 119906(119909 119905) for 120572 = ln 2 ln 3
provides the components of the exact solution which is localfractional continuous function where these componentsare also local fractional continuous functions Both thevariational iteration method and the decomposition methodwithin local fractional operators provide the solution insuccessive componentsThemethods are structured to get thelocal fractional series solution which is a nondifferentiablefunction
Conflict of Interests
The authors declare that there is no conflict of interestsregarding publication of this paper
References
[1] A M Wazwaz Partial Differential Equations Methods andApplications Elsevier Balkema The Netherlands 2002
[2] W R Schneider and W Wyss ldquoFractional diffusion and waveequationsrdquo Journal of Mathematical Physics vol 30 no 1 pp134ndash144 1989
[3] Z G Zhao and C P Li ldquoFractional differencefinite elementapproximations for the time-space fractional telegraph equa-tionrdquo Applied Mathematics and Computation vol 219 no 6 pp2975ndash2988 2012
[4] S Momani Z Odibat and A Alawneh ldquoVariational iterationmethod for solving the space- and time-fractional KdV equa-tionrdquo Numerical Methods for Partial Differential Equations vol24 no 1 pp 262ndash271 2008
[5] N Laskin ldquoFractional Schrodinger equationrdquo Physical ReviewE vol 66 Article ID 056108 2002
[6] Y Zhou and F Jiao ldquoNonlocal Cauchy problem for fractionalevolution equationsrdquo Nonlinear Analysis Real World Applica-tions vol 11 no 5 pp 4465ndash4475 2010
[7] S Momani and Z Odibat ldquoAnalytical solution of a time-fractional Navier-Stokes equation by Adomian decompositionmethodrdquo Applied Mathematics and Computation vol 177 no 2pp 488ndash494 2006
[8] V E Tarasov ldquoFractional Heisenberg equationrdquo Physics LettersA vol 372 no 17 pp 2984ndash2988 2008
[9] A K Golmankhaneh A K Golmankhaneh and D BaleanuldquoOn nonlinear fractional KleinGordon equationrdquo Signal Pro-cessing vol 91 no 3 pp 446ndash451 2011
[10] Z B Li W H Zhu and L L Huang ldquoApplication of fractionalvariational iteration method to time-fractional Fisher equa-tionrdquo Advanced Science Letters vol 10 no 1 pp 610ndash614 2012
[11] J Hristov ldquoHeat-balance integral to fractional (half-time) heatdiffusion sub-modelrdquoThermal Science vol 14 no 2 pp 291ndash3162010
[12] D Baleanu K Diethelm E Scalas and J J Trujillo FractionalCalculus Models and Numerical Methods vol 3 of Series onComplexity Nonlinearity and Chaos World Scientific BostonMass USA 2012
[13] C Cattani ldquoHarmonic wavelet solution of Poissonrsquos problemrdquoBalkan Journal of Geometry and Its Applications vol 13 no 1pp 27ndash37 2008
[14] C Cattani ldquoHarmonic wavelets towards the solution of nonlin-ear PDErdquo Computers amp Mathematics with Applications vol 50no 8-9 pp 1191ndash1210 2005
[15] X J Yang Local Fractional Functional Analysis and Its Applica-tions Asian Academic Hong Kong China 2011
[16] X J Yang and D Baleanu ldquoFractal heat conduction problemsolved by local fractional variation iteration methodrdquo ThermalScience vol 17 no 2 pp 625ndash628 2013
[17] W-H Su D Baleanu X-J Yang and H Jafari ldquoDamped waveequation and dissipative wave equation in fractal strings withinthe local fractional variational iteration methodrdquo Fixed PointTheory and Applications vol 2013 article 89 2013
[18] X J Yang D Baleanu and W P Zhong ldquoApproximation solu-tions for diffusion equation on Cantor time-spacerdquo Proceedingof the Romanian Academy A vol 14 no 2 pp 127ndash133 2013
[19] X J Yang D Baleanu and J A T Machado ldquoMathematicalaspects of Heisenberg uncertainty principle within local frac-tional Fourier analysisrdquoBoundary Value Problems no 1 pp 131ndash146 2013
[20] J Klafter S C Lim and RMetzler Fractional Dynamics RecentAdvances World Scientific Singapore 2012
[21] J Sabatier O P Agrawal and J T Machado Advances inFractional Calculus Theoretical Developments and Applicationsin Physics and Engineering Springer 2007
[22] R Hilfer Applications of Fractional Calculus in Physics WordScientific Singapore 2000
[23] M Li S C Lim and S Chen ldquoExact solution of impulseresponse to a class of fractional oscillators and its stabilityrdquoMathematical Problems in Engineering vol 2011 Article ID657839 9 pages 2011
[24] K M Kolwankar and A D Gangal ldquoLocal fractional Fokker-Planck equationrdquo Physical Review Letters vol 80 no 2 pp 214ndash217 1998
[25] K M Kolwankar and A D Gangal ldquoFractional differentiabilityof nowhere differentiable functions and dimensionsrdquo Chaosvol 6 no 4 pp 505ndash513 1996
[26] A Babakhani and V Daftardar-Gejji ldquoOn calculus of localfractional derivativesrdquo Journal of Mathematical Analysis andApplications vol 270 no 1 pp 66ndash79 2002
[27] Y Chen Y Yan and K Zhang ldquoOn the local fractionalderivativerdquo Journal of Mathematical Analysis and Applicationsvol 362 no 1 pp 17ndash33 2010
[28] A Carpinteri B Chiaia and P Cornetti ldquoStatic-kinematicduality and the principle of virtual work in the mechanics of
6 Abstract and Applied Analysis
fractal mediardquo Computer Methods in Applied Mechanics andEngineering vol 191 no 1-2 pp 3ndash19 2001
[29] A Carpinteri B Chiaia and P Cornetti ldquoThe elastic problemfor fractal media basic theory and finite element formulationrdquoComputers and Structures vol 82 no 6 pp 499ndash508 2004
[30] A Carpinteri and P Cornetti ldquoA fractional calculus approach tothe description of stress and strain localization in fractalmediardquoChaos Solitons amp Fractals vol 13 no 1 pp 85ndash94 2002
[31] F Ben Adda and J Cresson ldquoAbout non-differentiable func-tionsrdquo Journal of Mathematical Analysis and Applications vol263 no 2 pp 721ndash737 2001
[32] W Chen ldquoTime-space fabric underlying anomalous diffusionrdquoChaos Solitons amp Fractals vol 28 no 4 pp 923ndash929 2006
[33] W Chen H G Sun X D Zhang and D Korosak ldquoAnoma-lous diffusion modeling by fractal and fractional derivativesrdquoComputers amp Mathematics with Applications vol 59 no 5 pp1754ndash1758 2010
[34] G Jumarie ldquoModified Riemann-Liouville derivative and frac-tional Taylor series of nondifferentiable functions furtherresultsrdquoComputersampMathematics with Applications vol 51 no9-10 pp 1367ndash1376 2006
[35] X J Yang Advanced Local Fractional Calculus and Its Applica-tions World Science New York NY USA 2012
[36] A-M Yang X-J Yang and Z-B Li ldquoLocal fractional seriesexpansion method for solving wave and diffusion equations onCantor setsrdquoAbstract and Applied Analysis vol 2013 Article ID351057 5 pages 2013
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
Abstract and Applied Analysis 3
where 119899is considered as a restricted local fractional varia-
tion that is 120575120572119899= 0 (for more details see [35])
For 119899 = 2 we have
120582120572=
(119904 minus 119905)120572
Γ (1 + 120572) (13)
so that iteration is expressed as
119906119899+1
(119905) = 119906119899(119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)119871(119899)
120572119906119899(119904) + 119877
120572119906119899(119904) (119889119904)
120572
(14)
Finally the solution is
119906 (119909) = lim119899rarrinfin
119906119899(119909) (15)
32 Local Fractional Decomposition Method When 119871(119899)
120572in
(10) is a local fractional differential operator of order 2120572 wedenote it as
119871(119899)
120572= 119871(2120572)
119909119909=
1205972120572
1205971199092120572
119877120572119906 (119905) =
120597120572
120597119909120572119906 (119905) + 119891 (119905)
(16)
By defining the 119899-fold local fractional integral operator
119871(minus2)
120572119898(119904) =
0119868119909(120572)
0119868119909(120572)
119898(119904) (17)
we get
119871(minus2)
120572119871(2)
120572119906 (119904) = 119871
(minus2)
120572119877120572119906 (119904) (18)
Thus
119906 (119904) = 119903 (119909) + 119871(minus2)
120572119877120572119906 (119904) (19)
where the term 119903(119909) is to be determined from the fractalinitial conditions
Therefore we get the iterative formula as follows
119906 (119909) = 1199060(119909) + 119871
(minus2)
120572119877120572119906 (119904) (20)
with 1199060(119909) = 119903(119909)
Hence for 119899 ge 0 we have the following recurrencerelationship
119906119899+1
(119909) = 119871(minus2)
120572119877120572119906119899(119904)
1199060(119909) = 119903 (119909)
(21)
Finally the solution can be constructed as
119906 (119909) = lim119899rarrinfin
120601119899(119909) = lim
119899rarrinfin
infin
sum
119899=0
119906119899(119909) (22)
For more details see [18]
4 An Illustrative Example
In this section one example for wave equation is presented inorder to demonstrate the simplicity and the efficiency of theabove methods
In (2) we consider the following initial and boundaryconditions
120597120572119906 (119909 0)
120597119905120572= 0 119906 (119909 0) =
1199092120572
Γ (1 + 2120572) (23)
Using (14) we have the iterative formula
119906119899+1
(119909 119905)
= 119906119899(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1205972120572119906119899(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
1205972120572119906119899(119909 119904)
1205971199092120572(119889119904)120572
(24)
where the initial value is given by
1199060(119909 119905) =
1199092120572
Γ (1 + 2120572) (25)
Thus after computing (23) we obtain
1199061(119909 119905)
= 1199060(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199060(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
12059721205721199060(119909 119904)
1205971199092120572(119889119904)120572
= 1199060(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)(1 +
1199052120572
Γ (1 + 2120572))
1199062(119909 119905)
= 1199061(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199061(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
12059721205721199061(119909 119904)
1205971199092120572(119889119904)120572
= 1199061(119909 119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572)
1199042120572
Γ (1 + 2120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)(1 +
1199052120572
Γ (1 + 2120572)+
1199054120572
Γ (1 + 4120572))
4 Abstract and Applied Analysis
1199063(119909 119905)
= 1199062(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199062(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
12059721205721199062(119909 119904)
1205971199092120572(119889119904)120572
= 1199062(119909 119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572)
1199054120572
Γ (1 + 4120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)
3
sum
119894=0
1199052119894120572
Γ (1 + 2119894120572)
1199064(119909 119905)
= 1199063(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199063(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
1199092120572
Γ (1 + 2120572)
12059721205721199063(119909 119904)
1205971199092120572(119889119904)120572
= 1199063(119909 119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572)
1199056120572
Γ (1 + 6120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)
4
sum
119894=0
1199052119894120572
Γ (1 + 2119894120572)
(26)
119906119899(119909 119905)
= 119906119899minus1
(119909 119905) +1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1205972120572119906119899minus1
(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
1205972120572119906119899minus1
(119909 119904)
1205971199092120572(119889119904)120572
=1199092120572
Γ (1 + 2120572)
119899
sum
119894=0
1199052119894120572
Γ (1 + 2119894120572)
(27)
Hence from (27) we obtain the solution of (3) as
119906 (119909) = lim119899rarrinfin
119906119899(119909) =
1199092120572
Γ (1 + 2120572)cosh120572(119905120572) (28)
Here from (21) we get
119906119899+1
(119909 119905) =0119868119905(120572)
0119868119905(120572) 119909
2120572
Γ (1 + 2120572)
1205972120572119906119899(119909 119904)
1205971199092120572
1199060(119909 119905) =
1199092120572
Γ (1 + 2120572)
(29)
Therefore from (29) we give the components as follows
1199060(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199061(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199052120572
Γ (1 + 2120572)
1199062(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199054120572
Γ (1 + 4120572)
1199063(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199053120572
Γ (1 + 6120572)
1199064(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199058120572
Γ (1 + 8120572)
119906119899(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199052119899120572
Γ (1 + 2119899120572)
(30)
Consequently the exact solution is given by
119906 (119909 119905) = lim119899rarrinfin
infin
sum
119899=0
119906119899(119909 119905)
= lim119899rarrinfin
infin
sum
119899=0
1199092120572
Γ (1 + 2120572)
1199052119899120572
Γ (1 + 2119899120572)
=1199092120572
Γ (1 + 2120572)cosh120572(119909120572)
(31)
where
cosh120572(119909120572) =
infin
sum
119899=0
1199052119899120572
Γ (1 + 2119899120572) (32)
The solution of (2) for 120572 = ln 2 ln 3 is depicted in Figure 1
5 Conclusions
In this work we developed a comparison between thevariational iteration method and the decomposition methodwithin local fractional operators The two approaches con-stitute efficient tools to handle the approximation solutionsfor differential equations on Cantor sets with local fractionalderivative We notice that the fractional variational iterationmethod gives the several successive approximate formulasusing the iteration of the correction local fractional func-tional However the local fractional decomposition method
Abstract and Applied Analysis 5
25
2
15
1
05
01
05
0 002
0406
081
x
t
u(xt)
Figure 1 Graph of 119906(119909 119905) for 120572 = ln 2 ln 3
provides the components of the exact solution which is localfractional continuous function where these componentsare also local fractional continuous functions Both thevariational iteration method and the decomposition methodwithin local fractional operators provide the solution insuccessive componentsThemethods are structured to get thelocal fractional series solution which is a nondifferentiablefunction
Conflict of Interests
The authors declare that there is no conflict of interestsregarding publication of this paper
References
[1] A M Wazwaz Partial Differential Equations Methods andApplications Elsevier Balkema The Netherlands 2002
[2] W R Schneider and W Wyss ldquoFractional diffusion and waveequationsrdquo Journal of Mathematical Physics vol 30 no 1 pp134ndash144 1989
[3] Z G Zhao and C P Li ldquoFractional differencefinite elementapproximations for the time-space fractional telegraph equa-tionrdquo Applied Mathematics and Computation vol 219 no 6 pp2975ndash2988 2012
[4] S Momani Z Odibat and A Alawneh ldquoVariational iterationmethod for solving the space- and time-fractional KdV equa-tionrdquo Numerical Methods for Partial Differential Equations vol24 no 1 pp 262ndash271 2008
[5] N Laskin ldquoFractional Schrodinger equationrdquo Physical ReviewE vol 66 Article ID 056108 2002
[6] Y Zhou and F Jiao ldquoNonlocal Cauchy problem for fractionalevolution equationsrdquo Nonlinear Analysis Real World Applica-tions vol 11 no 5 pp 4465ndash4475 2010
[7] S Momani and Z Odibat ldquoAnalytical solution of a time-fractional Navier-Stokes equation by Adomian decompositionmethodrdquo Applied Mathematics and Computation vol 177 no 2pp 488ndash494 2006
[8] V E Tarasov ldquoFractional Heisenberg equationrdquo Physics LettersA vol 372 no 17 pp 2984ndash2988 2008
[9] A K Golmankhaneh A K Golmankhaneh and D BaleanuldquoOn nonlinear fractional KleinGordon equationrdquo Signal Pro-cessing vol 91 no 3 pp 446ndash451 2011
[10] Z B Li W H Zhu and L L Huang ldquoApplication of fractionalvariational iteration method to time-fractional Fisher equa-tionrdquo Advanced Science Letters vol 10 no 1 pp 610ndash614 2012
[11] J Hristov ldquoHeat-balance integral to fractional (half-time) heatdiffusion sub-modelrdquoThermal Science vol 14 no 2 pp 291ndash3162010
[12] D Baleanu K Diethelm E Scalas and J J Trujillo FractionalCalculus Models and Numerical Methods vol 3 of Series onComplexity Nonlinearity and Chaos World Scientific BostonMass USA 2012
[13] C Cattani ldquoHarmonic wavelet solution of Poissonrsquos problemrdquoBalkan Journal of Geometry and Its Applications vol 13 no 1pp 27ndash37 2008
[14] C Cattani ldquoHarmonic wavelets towards the solution of nonlin-ear PDErdquo Computers amp Mathematics with Applications vol 50no 8-9 pp 1191ndash1210 2005
[15] X J Yang Local Fractional Functional Analysis and Its Applica-tions Asian Academic Hong Kong China 2011
[16] X J Yang and D Baleanu ldquoFractal heat conduction problemsolved by local fractional variation iteration methodrdquo ThermalScience vol 17 no 2 pp 625ndash628 2013
[17] W-H Su D Baleanu X-J Yang and H Jafari ldquoDamped waveequation and dissipative wave equation in fractal strings withinthe local fractional variational iteration methodrdquo Fixed PointTheory and Applications vol 2013 article 89 2013
[18] X J Yang D Baleanu and W P Zhong ldquoApproximation solu-tions for diffusion equation on Cantor time-spacerdquo Proceedingof the Romanian Academy A vol 14 no 2 pp 127ndash133 2013
[19] X J Yang D Baleanu and J A T Machado ldquoMathematicalaspects of Heisenberg uncertainty principle within local frac-tional Fourier analysisrdquoBoundary Value Problems no 1 pp 131ndash146 2013
[20] J Klafter S C Lim and RMetzler Fractional Dynamics RecentAdvances World Scientific Singapore 2012
[21] J Sabatier O P Agrawal and J T Machado Advances inFractional Calculus Theoretical Developments and Applicationsin Physics and Engineering Springer 2007
[22] R Hilfer Applications of Fractional Calculus in Physics WordScientific Singapore 2000
[23] M Li S C Lim and S Chen ldquoExact solution of impulseresponse to a class of fractional oscillators and its stabilityrdquoMathematical Problems in Engineering vol 2011 Article ID657839 9 pages 2011
[24] K M Kolwankar and A D Gangal ldquoLocal fractional Fokker-Planck equationrdquo Physical Review Letters vol 80 no 2 pp 214ndash217 1998
[25] K M Kolwankar and A D Gangal ldquoFractional differentiabilityof nowhere differentiable functions and dimensionsrdquo Chaosvol 6 no 4 pp 505ndash513 1996
[26] A Babakhani and V Daftardar-Gejji ldquoOn calculus of localfractional derivativesrdquo Journal of Mathematical Analysis andApplications vol 270 no 1 pp 66ndash79 2002
[27] Y Chen Y Yan and K Zhang ldquoOn the local fractionalderivativerdquo Journal of Mathematical Analysis and Applicationsvol 362 no 1 pp 17ndash33 2010
[28] A Carpinteri B Chiaia and P Cornetti ldquoStatic-kinematicduality and the principle of virtual work in the mechanics of
6 Abstract and Applied Analysis
fractal mediardquo Computer Methods in Applied Mechanics andEngineering vol 191 no 1-2 pp 3ndash19 2001
[29] A Carpinteri B Chiaia and P Cornetti ldquoThe elastic problemfor fractal media basic theory and finite element formulationrdquoComputers and Structures vol 82 no 6 pp 499ndash508 2004
[30] A Carpinteri and P Cornetti ldquoA fractional calculus approach tothe description of stress and strain localization in fractalmediardquoChaos Solitons amp Fractals vol 13 no 1 pp 85ndash94 2002
[31] F Ben Adda and J Cresson ldquoAbout non-differentiable func-tionsrdquo Journal of Mathematical Analysis and Applications vol263 no 2 pp 721ndash737 2001
[32] W Chen ldquoTime-space fabric underlying anomalous diffusionrdquoChaos Solitons amp Fractals vol 28 no 4 pp 923ndash929 2006
[33] W Chen H G Sun X D Zhang and D Korosak ldquoAnoma-lous diffusion modeling by fractal and fractional derivativesrdquoComputers amp Mathematics with Applications vol 59 no 5 pp1754ndash1758 2010
[34] G Jumarie ldquoModified Riemann-Liouville derivative and frac-tional Taylor series of nondifferentiable functions furtherresultsrdquoComputersampMathematics with Applications vol 51 no9-10 pp 1367ndash1376 2006
[35] X J Yang Advanced Local Fractional Calculus and Its Applica-tions World Science New York NY USA 2012
[36] A-M Yang X-J Yang and Z-B Li ldquoLocal fractional seriesexpansion method for solving wave and diffusion equations onCantor setsrdquoAbstract and Applied Analysis vol 2013 Article ID351057 5 pages 2013
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
4 Abstract and Applied Analysis
1199063(119909 119905)
= 1199062(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199062(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
12059721205721199062(119909 119904)
1205971199092120572(119889119904)120572
= 1199062(119909 119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572)
1199054120572
Γ (1 + 4120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)
3
sum
119894=0
1199052119894120572
Γ (1 + 2119894120572)
1199064(119909 119905)
= 1199063(119909 119905) +
1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
12059721205721199063(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)int
119905
0
1199092120572
Γ (1 + 2120572)
12059721205721199063(119909 119904)
1205971199092120572(119889119904)120572
= 1199063(119909 119905) +
1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)minus
1199092120572
Γ (1 + 2120572)
1199056120572
Γ (1 + 6120572) (119889119904)
120572
=1199092120572
Γ (1 + 2120572)
4
sum
119894=0
1199052119894120572
Γ (1 + 2119894120572)
(26)
119906119899(119909 119905)
= 119906119899minus1
(119909 119905) +1
Γ (1 + 120572)int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1205972120572119906119899minus1
(119909 119904)
1205971199042120572(119889119904)120572
minus1
Γ (1 + 120572)
times int
119905
0
(119904 minus 119905)120572
Γ (1 + 120572)
1199092120572
Γ (1 + 2120572)
1205972120572119906119899minus1
(119909 119904)
1205971199092120572(119889119904)120572
=1199092120572
Γ (1 + 2120572)
119899
sum
119894=0
1199052119894120572
Γ (1 + 2119894120572)
(27)
Hence from (27) we obtain the solution of (3) as
119906 (119909) = lim119899rarrinfin
119906119899(119909) =
1199092120572
Γ (1 + 2120572)cosh120572(119905120572) (28)
Here from (21) we get
119906119899+1
(119909 119905) =0119868119905(120572)
0119868119905(120572) 119909
2120572
Γ (1 + 2120572)
1205972120572119906119899(119909 119904)
1205971199092120572
1199060(119909 119905) =
1199092120572
Γ (1 + 2120572)
(29)
Therefore from (29) we give the components as follows
1199060(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199061(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199052120572
Γ (1 + 2120572)
1199062(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199054120572
Γ (1 + 4120572)
1199063(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199053120572
Γ (1 + 6120572)
1199064(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199058120572
Γ (1 + 8120572)
119906119899(119909 119905) =
1199092120572
Γ (1 + 2120572)
1199052119899120572
Γ (1 + 2119899120572)
(30)
Consequently the exact solution is given by
119906 (119909 119905) = lim119899rarrinfin
infin
sum
119899=0
119906119899(119909 119905)
= lim119899rarrinfin
infin
sum
119899=0
1199092120572
Γ (1 + 2120572)
1199052119899120572
Γ (1 + 2119899120572)
=1199092120572
Γ (1 + 2120572)cosh120572(119909120572)
(31)
where
cosh120572(119909120572) =
infin
sum
119899=0
1199052119899120572
Γ (1 + 2119899120572) (32)
The solution of (2) for 120572 = ln 2 ln 3 is depicted in Figure 1
5 Conclusions
In this work we developed a comparison between thevariational iteration method and the decomposition methodwithin local fractional operators The two approaches con-stitute efficient tools to handle the approximation solutionsfor differential equations on Cantor sets with local fractionalderivative We notice that the fractional variational iterationmethod gives the several successive approximate formulasusing the iteration of the correction local fractional func-tional However the local fractional decomposition method
Abstract and Applied Analysis 5
25
2
15
1
05
01
05
0 002
0406
081
x
t
u(xt)
Figure 1 Graph of 119906(119909 119905) for 120572 = ln 2 ln 3
provides the components of the exact solution which is localfractional continuous function where these componentsare also local fractional continuous functions Both thevariational iteration method and the decomposition methodwithin local fractional operators provide the solution insuccessive componentsThemethods are structured to get thelocal fractional series solution which is a nondifferentiablefunction
Conflict of Interests
The authors declare that there is no conflict of interestsregarding publication of this paper
References
[1] A M Wazwaz Partial Differential Equations Methods andApplications Elsevier Balkema The Netherlands 2002
[2] W R Schneider and W Wyss ldquoFractional diffusion and waveequationsrdquo Journal of Mathematical Physics vol 30 no 1 pp134ndash144 1989
[3] Z G Zhao and C P Li ldquoFractional differencefinite elementapproximations for the time-space fractional telegraph equa-tionrdquo Applied Mathematics and Computation vol 219 no 6 pp2975ndash2988 2012
[4] S Momani Z Odibat and A Alawneh ldquoVariational iterationmethod for solving the space- and time-fractional KdV equa-tionrdquo Numerical Methods for Partial Differential Equations vol24 no 1 pp 262ndash271 2008
[5] N Laskin ldquoFractional Schrodinger equationrdquo Physical ReviewE vol 66 Article ID 056108 2002
[6] Y Zhou and F Jiao ldquoNonlocal Cauchy problem for fractionalevolution equationsrdquo Nonlinear Analysis Real World Applica-tions vol 11 no 5 pp 4465ndash4475 2010
[7] S Momani and Z Odibat ldquoAnalytical solution of a time-fractional Navier-Stokes equation by Adomian decompositionmethodrdquo Applied Mathematics and Computation vol 177 no 2pp 488ndash494 2006
[8] V E Tarasov ldquoFractional Heisenberg equationrdquo Physics LettersA vol 372 no 17 pp 2984ndash2988 2008
[9] A K Golmankhaneh A K Golmankhaneh and D BaleanuldquoOn nonlinear fractional KleinGordon equationrdquo Signal Pro-cessing vol 91 no 3 pp 446ndash451 2011
[10] Z B Li W H Zhu and L L Huang ldquoApplication of fractionalvariational iteration method to time-fractional Fisher equa-tionrdquo Advanced Science Letters vol 10 no 1 pp 610ndash614 2012
[11] J Hristov ldquoHeat-balance integral to fractional (half-time) heatdiffusion sub-modelrdquoThermal Science vol 14 no 2 pp 291ndash3162010
[12] D Baleanu K Diethelm E Scalas and J J Trujillo FractionalCalculus Models and Numerical Methods vol 3 of Series onComplexity Nonlinearity and Chaos World Scientific BostonMass USA 2012
[13] C Cattani ldquoHarmonic wavelet solution of Poissonrsquos problemrdquoBalkan Journal of Geometry and Its Applications vol 13 no 1pp 27ndash37 2008
[14] C Cattani ldquoHarmonic wavelets towards the solution of nonlin-ear PDErdquo Computers amp Mathematics with Applications vol 50no 8-9 pp 1191ndash1210 2005
[15] X J Yang Local Fractional Functional Analysis and Its Applica-tions Asian Academic Hong Kong China 2011
[16] X J Yang and D Baleanu ldquoFractal heat conduction problemsolved by local fractional variation iteration methodrdquo ThermalScience vol 17 no 2 pp 625ndash628 2013
[17] W-H Su D Baleanu X-J Yang and H Jafari ldquoDamped waveequation and dissipative wave equation in fractal strings withinthe local fractional variational iteration methodrdquo Fixed PointTheory and Applications vol 2013 article 89 2013
[18] X J Yang D Baleanu and W P Zhong ldquoApproximation solu-tions for diffusion equation on Cantor time-spacerdquo Proceedingof the Romanian Academy A vol 14 no 2 pp 127ndash133 2013
[19] X J Yang D Baleanu and J A T Machado ldquoMathematicalaspects of Heisenberg uncertainty principle within local frac-tional Fourier analysisrdquoBoundary Value Problems no 1 pp 131ndash146 2013
[20] J Klafter S C Lim and RMetzler Fractional Dynamics RecentAdvances World Scientific Singapore 2012
[21] J Sabatier O P Agrawal and J T Machado Advances inFractional Calculus Theoretical Developments and Applicationsin Physics and Engineering Springer 2007
[22] R Hilfer Applications of Fractional Calculus in Physics WordScientific Singapore 2000
[23] M Li S C Lim and S Chen ldquoExact solution of impulseresponse to a class of fractional oscillators and its stabilityrdquoMathematical Problems in Engineering vol 2011 Article ID657839 9 pages 2011
[24] K M Kolwankar and A D Gangal ldquoLocal fractional Fokker-Planck equationrdquo Physical Review Letters vol 80 no 2 pp 214ndash217 1998
[25] K M Kolwankar and A D Gangal ldquoFractional differentiabilityof nowhere differentiable functions and dimensionsrdquo Chaosvol 6 no 4 pp 505ndash513 1996
[26] A Babakhani and V Daftardar-Gejji ldquoOn calculus of localfractional derivativesrdquo Journal of Mathematical Analysis andApplications vol 270 no 1 pp 66ndash79 2002
[27] Y Chen Y Yan and K Zhang ldquoOn the local fractionalderivativerdquo Journal of Mathematical Analysis and Applicationsvol 362 no 1 pp 17ndash33 2010
[28] A Carpinteri B Chiaia and P Cornetti ldquoStatic-kinematicduality and the principle of virtual work in the mechanics of
6 Abstract and Applied Analysis
fractal mediardquo Computer Methods in Applied Mechanics andEngineering vol 191 no 1-2 pp 3ndash19 2001
[29] A Carpinteri B Chiaia and P Cornetti ldquoThe elastic problemfor fractal media basic theory and finite element formulationrdquoComputers and Structures vol 82 no 6 pp 499ndash508 2004
[30] A Carpinteri and P Cornetti ldquoA fractional calculus approach tothe description of stress and strain localization in fractalmediardquoChaos Solitons amp Fractals vol 13 no 1 pp 85ndash94 2002
[31] F Ben Adda and J Cresson ldquoAbout non-differentiable func-tionsrdquo Journal of Mathematical Analysis and Applications vol263 no 2 pp 721ndash737 2001
[32] W Chen ldquoTime-space fabric underlying anomalous diffusionrdquoChaos Solitons amp Fractals vol 28 no 4 pp 923ndash929 2006
[33] W Chen H G Sun X D Zhang and D Korosak ldquoAnoma-lous diffusion modeling by fractal and fractional derivativesrdquoComputers amp Mathematics with Applications vol 59 no 5 pp1754ndash1758 2010
[34] G Jumarie ldquoModified Riemann-Liouville derivative and frac-tional Taylor series of nondifferentiable functions furtherresultsrdquoComputersampMathematics with Applications vol 51 no9-10 pp 1367ndash1376 2006
[35] X J Yang Advanced Local Fractional Calculus and Its Applica-tions World Science New York NY USA 2012
[36] A-M Yang X-J Yang and Z-B Li ldquoLocal fractional seriesexpansion method for solving wave and diffusion equations onCantor setsrdquoAbstract and Applied Analysis vol 2013 Article ID351057 5 pages 2013
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
Abstract and Applied Analysis 5
25
2
15
1
05
01
05
0 002
0406
081
x
t
u(xt)
Figure 1 Graph of 119906(119909 119905) for 120572 = ln 2 ln 3
provides the components of the exact solution which is localfractional continuous function where these componentsare also local fractional continuous functions Both thevariational iteration method and the decomposition methodwithin local fractional operators provide the solution insuccessive componentsThemethods are structured to get thelocal fractional series solution which is a nondifferentiablefunction
Conflict of Interests
The authors declare that there is no conflict of interestsregarding publication of this paper
References
[1] A M Wazwaz Partial Differential Equations Methods andApplications Elsevier Balkema The Netherlands 2002
[2] W R Schneider and W Wyss ldquoFractional diffusion and waveequationsrdquo Journal of Mathematical Physics vol 30 no 1 pp134ndash144 1989
[3] Z G Zhao and C P Li ldquoFractional differencefinite elementapproximations for the time-space fractional telegraph equa-tionrdquo Applied Mathematics and Computation vol 219 no 6 pp2975ndash2988 2012
[4] S Momani Z Odibat and A Alawneh ldquoVariational iterationmethod for solving the space- and time-fractional KdV equa-tionrdquo Numerical Methods for Partial Differential Equations vol24 no 1 pp 262ndash271 2008
[5] N Laskin ldquoFractional Schrodinger equationrdquo Physical ReviewE vol 66 Article ID 056108 2002
[6] Y Zhou and F Jiao ldquoNonlocal Cauchy problem for fractionalevolution equationsrdquo Nonlinear Analysis Real World Applica-tions vol 11 no 5 pp 4465ndash4475 2010
[7] S Momani and Z Odibat ldquoAnalytical solution of a time-fractional Navier-Stokes equation by Adomian decompositionmethodrdquo Applied Mathematics and Computation vol 177 no 2pp 488ndash494 2006
[8] V E Tarasov ldquoFractional Heisenberg equationrdquo Physics LettersA vol 372 no 17 pp 2984ndash2988 2008
[9] A K Golmankhaneh A K Golmankhaneh and D BaleanuldquoOn nonlinear fractional KleinGordon equationrdquo Signal Pro-cessing vol 91 no 3 pp 446ndash451 2011
[10] Z B Li W H Zhu and L L Huang ldquoApplication of fractionalvariational iteration method to time-fractional Fisher equa-tionrdquo Advanced Science Letters vol 10 no 1 pp 610ndash614 2012
[11] J Hristov ldquoHeat-balance integral to fractional (half-time) heatdiffusion sub-modelrdquoThermal Science vol 14 no 2 pp 291ndash3162010
[12] D Baleanu K Diethelm E Scalas and J J Trujillo FractionalCalculus Models and Numerical Methods vol 3 of Series onComplexity Nonlinearity and Chaos World Scientific BostonMass USA 2012
[13] C Cattani ldquoHarmonic wavelet solution of Poissonrsquos problemrdquoBalkan Journal of Geometry and Its Applications vol 13 no 1pp 27ndash37 2008
[14] C Cattani ldquoHarmonic wavelets towards the solution of nonlin-ear PDErdquo Computers amp Mathematics with Applications vol 50no 8-9 pp 1191ndash1210 2005
[15] X J Yang Local Fractional Functional Analysis and Its Applica-tions Asian Academic Hong Kong China 2011
[16] X J Yang and D Baleanu ldquoFractal heat conduction problemsolved by local fractional variation iteration methodrdquo ThermalScience vol 17 no 2 pp 625ndash628 2013
[17] W-H Su D Baleanu X-J Yang and H Jafari ldquoDamped waveequation and dissipative wave equation in fractal strings withinthe local fractional variational iteration methodrdquo Fixed PointTheory and Applications vol 2013 article 89 2013
[18] X J Yang D Baleanu and W P Zhong ldquoApproximation solu-tions for diffusion equation on Cantor time-spacerdquo Proceedingof the Romanian Academy A vol 14 no 2 pp 127ndash133 2013
[19] X J Yang D Baleanu and J A T Machado ldquoMathematicalaspects of Heisenberg uncertainty principle within local frac-tional Fourier analysisrdquoBoundary Value Problems no 1 pp 131ndash146 2013
[20] J Klafter S C Lim and RMetzler Fractional Dynamics RecentAdvances World Scientific Singapore 2012
[21] J Sabatier O P Agrawal and J T Machado Advances inFractional Calculus Theoretical Developments and Applicationsin Physics and Engineering Springer 2007
[22] R Hilfer Applications of Fractional Calculus in Physics WordScientific Singapore 2000
[23] M Li S C Lim and S Chen ldquoExact solution of impulseresponse to a class of fractional oscillators and its stabilityrdquoMathematical Problems in Engineering vol 2011 Article ID657839 9 pages 2011
[24] K M Kolwankar and A D Gangal ldquoLocal fractional Fokker-Planck equationrdquo Physical Review Letters vol 80 no 2 pp 214ndash217 1998
[25] K M Kolwankar and A D Gangal ldquoFractional differentiabilityof nowhere differentiable functions and dimensionsrdquo Chaosvol 6 no 4 pp 505ndash513 1996
[26] A Babakhani and V Daftardar-Gejji ldquoOn calculus of localfractional derivativesrdquo Journal of Mathematical Analysis andApplications vol 270 no 1 pp 66ndash79 2002
[27] Y Chen Y Yan and K Zhang ldquoOn the local fractionalderivativerdquo Journal of Mathematical Analysis and Applicationsvol 362 no 1 pp 17ndash33 2010
[28] A Carpinteri B Chiaia and P Cornetti ldquoStatic-kinematicduality and the principle of virtual work in the mechanics of
6 Abstract and Applied Analysis
fractal mediardquo Computer Methods in Applied Mechanics andEngineering vol 191 no 1-2 pp 3ndash19 2001
[29] A Carpinteri B Chiaia and P Cornetti ldquoThe elastic problemfor fractal media basic theory and finite element formulationrdquoComputers and Structures vol 82 no 6 pp 499ndash508 2004
[30] A Carpinteri and P Cornetti ldquoA fractional calculus approach tothe description of stress and strain localization in fractalmediardquoChaos Solitons amp Fractals vol 13 no 1 pp 85ndash94 2002
[31] F Ben Adda and J Cresson ldquoAbout non-differentiable func-tionsrdquo Journal of Mathematical Analysis and Applications vol263 no 2 pp 721ndash737 2001
[32] W Chen ldquoTime-space fabric underlying anomalous diffusionrdquoChaos Solitons amp Fractals vol 28 no 4 pp 923ndash929 2006
[33] W Chen H G Sun X D Zhang and D Korosak ldquoAnoma-lous diffusion modeling by fractal and fractional derivativesrdquoComputers amp Mathematics with Applications vol 59 no 5 pp1754ndash1758 2010
[34] G Jumarie ldquoModified Riemann-Liouville derivative and frac-tional Taylor series of nondifferentiable functions furtherresultsrdquoComputersampMathematics with Applications vol 51 no9-10 pp 1367ndash1376 2006
[35] X J Yang Advanced Local Fractional Calculus and Its Applica-tions World Science New York NY USA 2012
[36] A-M Yang X-J Yang and Z-B Li ldquoLocal fractional seriesexpansion method for solving wave and diffusion equations onCantor setsrdquoAbstract and Applied Analysis vol 2013 Article ID351057 5 pages 2013
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
6 Abstract and Applied Analysis
fractal mediardquo Computer Methods in Applied Mechanics andEngineering vol 191 no 1-2 pp 3ndash19 2001
[29] A Carpinteri B Chiaia and P Cornetti ldquoThe elastic problemfor fractal media basic theory and finite element formulationrdquoComputers and Structures vol 82 no 6 pp 499ndash508 2004
[30] A Carpinteri and P Cornetti ldquoA fractional calculus approach tothe description of stress and strain localization in fractalmediardquoChaos Solitons amp Fractals vol 13 no 1 pp 85ndash94 2002
[31] F Ben Adda and J Cresson ldquoAbout non-differentiable func-tionsrdquo Journal of Mathematical Analysis and Applications vol263 no 2 pp 721ndash737 2001
[32] W Chen ldquoTime-space fabric underlying anomalous diffusionrdquoChaos Solitons amp Fractals vol 28 no 4 pp 923ndash929 2006
[33] W Chen H G Sun X D Zhang and D Korosak ldquoAnoma-lous diffusion modeling by fractal and fractional derivativesrdquoComputers amp Mathematics with Applications vol 59 no 5 pp1754ndash1758 2010
[34] G Jumarie ldquoModified Riemann-Liouville derivative and frac-tional Taylor series of nondifferentiable functions furtherresultsrdquoComputersampMathematics with Applications vol 51 no9-10 pp 1367ndash1376 2006
[35] X J Yang Advanced Local Fractional Calculus and Its Applica-tions World Science New York NY USA 2012
[36] A-M Yang X-J Yang and Z-B Li ldquoLocal fractional seriesexpansion method for solving wave and diffusion equations onCantor setsrdquoAbstract and Applied Analysis vol 2013 Article ID351057 5 pages 2013
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of