scieee Science in your language
[en] (orig)

Existence results for a coupled system of nonlinear singular fractional differential equations with impulse effects

Abstract

A boundary value problem for the singular fractional differential system with impulse effects is presented. By applying Schauder's fixed point theorem in a suitably Banach space, we obtain the existence of at least one solution for this problem. Two examples are presented to illustrate the main theorem

Read accessible full text

Existence results for a coupled system of nonlinear singular fractional differential equations with impulse effects

Author: Liu, Yuji; Nieto Roig, Juan José; Otero Zarraquiños, Óscar Alejandro
Publisher: Hindawi
Year: 2013
DOI: 10.1155/2013/498781
Source: https://minerva.usc.es/bitstreams/0b464f45-cd88-471b-a59d-c201c75f3605/download
Hindawi Publishing Co po a ion
Ma hema ical P oblems in Enginee ing
Volume 2013, A icle ID 498781, 21 pages
h p://dx.doi.o g/10.1155/2013/498781
Resea ch A icle
Exis ence Resul s o a Coupled Sys em o Nonlinea Singula
F ac ional Di e en ial Equa ions wi h Impulse E ec s
Yuji Liu,1Juan J. Nie o,2,3 and Ósca O e o-Za aquiños2
1Depa men o Ma hema ics, Guangdong Uni e si y o Business S udies, Guangzhou 510320, China
2Depa amen o de An´
alisis Ma em´
a ico, Facul ad de Ma em´
a icas, Uni e sidad de San iago de Compos ela,
15782 San iago de Compos ela, Spain
3Depa men o Ma hema ics, Facul y o Science, King Abdulaziz Uni e si y, P.O. Box 80203, Jeddah 21589, Saudi A abia
Co espondence should be add essed o Juan J. Nie o; juanjose.nie o[email p o ec ed]
Recei ed 2 Oc obe 2012; Accep ed 15 Feb ua y 2013
Academic Edi o : Jocelyn Saba ie
Copy igh © 2013 Yuji Liu e al. This is an open access a icle dis ibu ed unde he C ea i e Commons A ibu ion License, which
pe mi s un es ic ed use, dis ibu ion, and ep oduc ion in any medium, p o ided he o iginal wo k is p ope ly ci ed.
A bounda y alue p oblem o he singula ac ional di e en ial sys em wi h impulse e ec s is p esen ed. By applying Schaude ’s
ixed poin heo em in a sui ably Banach space, we ob ain he exis ence o a leas one solu ion o his p oblem. Two examples a e
p esen ed o illus a e he main heo em.
1. In oduc ion
F ac ional di e en ial equa ions ha e ecei ed inc easing
a en ion du ing ecen yea s since he beha io o many
physical, chemical, and enginee ing p ocesses can be p ope ly
desc ibed by using ac ional di e en ial equa ions heo y;
see he books [1–3], pape s [4,5] and e e ences he ein. Fo
de ails on he geome ic and physical in e p e a ion o he
de i a i es o nonin ege o de , see, o example, [6–11]. Fo
some ecen wo ks wi h applica ions o enginee ing we e e
he eade o [12–15].
Fo an in oduc ion o he basic heo y o impulsi e
di e en ial equa ion, we e e he eade o [16]. Among
p e ious esea ch, li le is conce ned wi h di e en ial equa-
ions wi h ac ional o de wi h impulses [17]. Ahmad and
Si asunda am [18,19] ga e some exis ence esul s o wo-
poin bounda y alue p oblems in ol ing nonlinea impul-
si e hyb id di e en ial equa ions o ac ional o de 1<
𝛼≤2. Ahmad and Nie o in [20] es ablish su icien
condi ions o he exis ence o solu ions o he an ipe iodic
bounda y alue p oblem o impulsi e di e en ial equa ions
wi h he Capu o de i a i e o o de 𝑞 ∈ (1,2].Some ecen
esul s on impulsi e ini ial alue p oblems o bounda y alue
p oblems o ac ional di e en ial equa ions on a ini e
in e alcanbe oundin[21–23] and e e ences he ein. The
memo y p ope y o ac ional calculus makes s udies mo e
complica ed.
This pape is mo i a ed by [24]inwhich he ollowing
bounda y alue p oblem o he ac ional di e en ial equa-
ion 𝐷𝛼
0+𝑥(𝑡)=𝑓(𝑡,𝑦(𝑡),𝐷𝑝
0+𝑦(𝑡)), 𝑡∈(0,1),
𝐷𝛽
0+𝑦(𝑡)=𝑔(𝑡,𝑥(𝑡),𝐷𝑞
0+𝑥(𝑡)), 𝑡∈(0,1),
𝑥(0)=0, 𝑦(0)=0, 𝑥(1)−𝛾𝑥(𝜂)=0,
𝑦(1)−𝛾𝑦(𝜂)=0
(1)
was s udied, whe e 1<𝛼,𝛽<2,0<𝑝≤𝛽−1and 0<
𝑞≤𝛼−1,𝛾>0,1>𝛾𝜂
𝛼−1,1>𝛾𝜂
𝛽−1 and 𝑓,𝑔 : [0,1]×
𝑅2→𝑅a e con inuous unc ions, and 𝐷0+is he Riemann-
Liou ille ac ional de i a i e. An exis ence esul was p o ed
o BVP (1)in[24]. The g ow h assump ions imposed on 𝑓
and 𝑔a e sublinea cases (see [25, Theo em 3.1]); ha is, he e
exis unc ions 𝑎,𝑏∈𝐿1(0,1), nonnega i e cons an s 𝜖1,𝜖2>
0,𝛿1,𝛿2≥0and 𝜌1,𝜌2,𝜎1,𝜎2∈(0,1)such ha
󵄨󵄨󵄨󵄨𝑓(𝑡,𝑥,𝑦)󵄨󵄨󵄨󵄨≤𝑎(𝑡)+𝜖1|𝑥|𝜌1+𝜖2󵄨󵄨󵄨󵄨𝑦󵄨󵄨󵄨󵄨𝜌2,
󵄨󵄨󵄨󵄨𝑔(𝑡,𝑥,𝑦)󵄨󵄨󵄨󵄨≤𝑏(𝑡)+𝛿1|𝑥|𝜎1+𝛿2󵄨󵄨󵄨󵄨𝑦󵄨󵄨󵄨󵄨𝜎2.(2)
2Ma hema ical P oblems in Enginee ing
In [25], he ollowing bounda y alue p oblem o he
ac ional di e en ial equa ion
𝐷𝛼
0+𝑥(𝑡)=𝑓(𝑡,𝑦(𝑡),𝐷𝑝
0+𝑦(𝑡)), 𝑡∈(0,1),
𝐷𝛽
0+𝑦(𝑡)=𝑔(𝑡,𝑥(𝑡),𝐷𝑞
0+𝑥(𝑡)), 𝑡∈(0,1),
𝑥(0)=0, 𝑦(0)=0, 𝑥(1)=0, 𝑦(1)=0
(3)
was s udied, whe e 1<𝛼,𝛽<2,0<𝑝≤𝛽−1and 0<𝑞≤
𝛼−1,and𝑓,𝑔 : [0,1]×𝑅2→𝑅a e con inuous unc ions,
and 𝐷0+is he Riemann-Liou ille ac ional de i a i e. The
g ow h assump ions imposed on 𝑓and 𝑔a e sublinea cases
(see [25, Theo em 3.1]), ha is, he e exis unc ions 𝑎,𝑏 ∈
𝐿1(0,1), nonnega i e cons an s 𝜖1,𝜖2>0,𝛿1,𝛿2≥0,and
𝜌1,𝜌2,𝜎1,𝜎2∈(0,1]such ha
󵄨󵄨󵄨󵄨𝑓(𝑡,𝑥,𝑦)󵄨󵄨󵄨󵄨≤𝑎(𝑡)+𝜖1|𝑥|𝜌1+𝜖2󵄨󵄨󵄨󵄨𝑦󵄨󵄨󵄨󵄨𝜌2,
󵄨󵄨󵄨󵄨𝑔(𝑡,𝑥,𝑦)󵄨󵄨󵄨󵄨≤𝑏(𝑡)+𝛿1|𝑥|𝜎1+𝛿2󵄨󵄨󵄨󵄨𝑦󵄨󵄨󵄨󵄨𝜎2,(4)
o sublinea cases, ha is, he e exis nonnega i e cons an s
𝜖1,𝜖2>0,𝛿1,𝛿2≥0and 𝜌1,𝜌2,𝜎1,𝜎2∈(1,∞)such ha
󵄨󵄨󵄨󵄨𝑓(𝑡,𝑥,𝑦)󵄨󵄨󵄨󵄨≤𝜖1|𝑥|𝜌1+𝜖2󵄨󵄨󵄨󵄨𝑦󵄨󵄨󵄨󵄨𝜌2,
󵄨󵄨󵄨󵄨𝑔(𝑡,𝑥,𝑦)󵄨󵄨󵄨󵄨≤𝛿1|𝑥|𝜎1+𝛿2󵄨󵄨󵄨󵄨𝑦󵄨󵄨󵄨󵄨𝜎2.(5)
We ind ha in he supe linea cases, BVP (3)hasapai o
solu ions (𝑥,𝑦)=(0,0)wi hou needing any o he assump-
ions. Hence, hese cases a e i ial ones discussed in [25].
I is in e es ing o conside he sol abili y o BVP (1)when
he g ow h assump ions imposed on 𝑓,𝑔 a e supe linea
cases. Fu he mo e, he sol abili y o BVP (1)isno s udied
when 𝑞>𝛼−1o 𝑝>𝛽−1.
In his pape we conside he ollowing nonlinea bound-
a y alue p oblem o he singula mul i e m ac ional
di e en ial equa ion wi h impulse e ec s whose bounda y
condi ions a e o in eg al o m
𝐷𝛼
0+𝑥(𝑡)=𝜙(𝑡)𝑓(𝑡,𝑦(𝑡),𝐷𝑝
0+𝑦(𝑡)),
𝑡∈(0,1),𝑡=𝑡1,
𝐷𝛽
0+𝑦(𝑡)=𝜓(𝑡)𝑔(𝑡,𝑥(𝑡),𝐷𝑞
0+𝑥(𝑡)),
𝑡∈(0,1),𝑡=𝑡1,
lim
𝑡→0𝑡2−𝛼𝑥(𝑡)=∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠,
lim
𝑡→0𝑡2−𝛽𝑦(𝑡)=∫1
0
V(𝑠)𝐻(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠,
𝑥(1)=∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠,
(6)
𝑦(1)=∫1
0𝑛(𝑠)𝑁(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠,
Δ𝑥(𝑡1)=lim
𝑡→𝑡+
1𝑥(𝑡)−lim
𝑡→𝑡−
1𝑥(𝑡)=𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)),
Δ𝑦(𝑡1)=lim
𝑡→𝑡+
1𝑦(𝑡)−lim
𝑡→𝑡−
1𝑦(𝑡)=𝐽(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1)),
Δ𝐷𝑞
0+𝑥(𝑡1)=lim
𝑡→𝑡+
1𝐷𝑞
0+𝑥(𝑡)−lim
𝑡→𝑡−
1𝐷𝑞
0+𝑥(𝑡)
=𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)),
Δ𝐷𝑝
0+𝑦(𝑡1)=lim
𝑡→𝑡+
1𝐷𝑝
0+𝑦(𝑡)−lim
𝑡→𝑡−
1𝐷𝑝
0+𝑦(𝑡)
=𝐽1(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1)), (7)
whe e
(a) 1<𝛼,𝛽≤2,0<𝑝<𝛽and 0<𝑞<𝛼,𝐷0+is he
Riemann-Liou ille ac ional de i a i e,
(b) 𝜙,𝜓:(0,1) → 𝑅,𝑓,𝑔de ined on (0,1)×𝑅2,
(c) 𝑚,𝑛,𝑢,V: (0,1) → 𝑅wi h 𝑚,𝑛,𝑢,V∈𝐿
1(0,1),
𝐺,𝐻,𝑀,𝑁de ined on (0,1)×𝑅2,
(d) 0=𝑡0<𝑡1<𝑡2=1,
(e) 𝐼,𝐼1,𝐽,𝐽1:(0,1)×𝑅2→𝑅.
Apai o unc ions(𝑥,𝑦)de ined on (0,1)is called a
solu ion o BVP (1)andBVP(3), i 𝑥|(𝑡𝑘,𝑡𝑘+1],𝐷𝑞
0+𝑥|(𝑡𝑘,𝑡𝑘+1]and
𝑦|(𝑡𝑘,𝑡𝑘+1],𝐷𝑝
0+𝑦|(𝑡𝑘,𝑡𝑘+1](𝑘 = 0,1)a e con inuous, he e exis s
he limi s
lim
𝑡→𝑡+
𝑘𝑡2−𝛼𝑥(𝑡),lim
𝑡→𝑡+
𝑘𝑡2−𝛽𝑦(𝑡),
lim
𝑡→𝑡+
𝑘𝑡2+𝑞−𝛼𝐷𝑞
0+𝑥(𝑡),lim
𝑡→𝑡+
𝑘𝑡2+𝑝−𝛽𝐷𝑝
0+𝑦(𝑡),
𝑘=0,1,
(8)
𝐷𝛼
0+𝑥,𝐷𝛽
0+𝑦∈𝐿1(0,1)and (𝑥,𝑦)sa is ies all equa ions in (6)
and (7).
The no el y o his pape is as ollows: i s , he ac ional
di e en ial equa ions in (6) a e mul i e m ones and hei
nonlinea i ies 𝑓,𝑔depend on he lowe ac ional de i a i es;
second, bo h 𝜙and 𝜓may be singula a 𝑡=0and
𝑡=1, ha is,𝜙(𝑡)𝑓(𝑡,𝑥,𝑦)and 𝜓(𝑡)𝑔(𝑡,𝑥,𝑦)may be no
con inuous unc ions on [0,1]×𝑅2, hebounda ycondi ions
a e in eg al bounda y condi ions, and we ob ain he esul s
on he exis ence o a leas one solu ion o BVP (6)-(7); hi d,
0<𝑝<𝛽and 0<𝑞<𝛼a esupposed; heg ow h
assump ions imposed on 𝑓,𝑔,𝐺,𝐻,𝑀,𝑁 and 𝐼,𝐼1,𝐽,𝐽1a e
allowed o be sublinea cases. Finally, wo examples a e gi en
o illus a e he e iciency o he main heo em.
The emainde o his pape is as ollows: in Sec ion 2,we
p esen p elimina y esul s. In Sec ion 3, hemain heo em
and i s p oo a e gi en. In Sec ion 4, wo examples a e gi en
o illus a e he main esul s.
Ma hema ical P oblems in Enginee ing 3
2. P elimina ies
In his sec ion, we p esen some backg ound de ini ions and
p elimina y esul s.
De ini ion 1 (see [1]). The Riemann-Liou ille ac ional in e-
g al o o de 𝛼>0o a unc ion 𝑔:(0,∞)→𝑅is gi en
by
𝐼𝛼
0+𝑔(𝑡)=1
Γ(𝛼)∫𝑡
0(𝑡−𝑠)𝛼−1𝑔(𝑠)𝑑𝑠, (9)
p o ided ha he igh -hand side exis s.
De ini ion 2 (see [1]). The Riemann-Liou ille ac ional
de i a i e o o de 𝛼>0o a con inuous unc ion 𝑔:
(0,∞) → 𝑅is gi en by
𝐷𝛼
0+𝑔(𝑡)=1
Γ(𝑛−𝛼)𝑑𝑛
𝑑𝑡𝑛∫𝑡
0𝑔(𝑠)
(𝑡−𝑠)𝛼−𝑛+1 𝑑𝑠, (10)
whe e 𝑛−1≤𝛼<𝑛, p o ided ha he igh -hand side is
poin wise de ined on (0,∞).
De ini ion 3. 𝐾:(0,1)×𝑅2→𝑅is called a 𝛽-Ca a heodo y
unc ion i 𝐾sa is ies ha
(i) 𝑡→𝐾(𝑡,𝑡
𝛽−2𝑈,𝑡𝛽−𝑝−2𝑉) is con inuous on
(𝑡𝑘,𝑡𝑘+1](𝑘=0,1) o e e y (𝑈,𝑉)∈𝑅2;
(ii) (𝑈,𝑉) → 𝐾(𝑡,𝑡𝛽−2𝑈,𝑡𝛽−𝑝−2𝑉)is con inuous on 𝑅2
o e e y 𝑡∈(0,1);
(iii) o each 𝑟>0 he e exis s a cons an 𝐴𝑟>0such ha
|𝐾(𝑡,𝑡𝛽−2𝑈,𝑡𝛽−𝑝−2𝑉)|≤𝐴𝑟,𝑡∈(0,1),|𝑈|,|𝑉|≤𝑟.
De ini ion 4. 𝑄:(0,1)×𝑅2→𝑅is called a 𝛼-Ca a heodo y
unc ion i 𝑄sa is ies ha
(i) 𝑡→𝑄(𝑡,𝑡
𝛼−2𝑈,𝑡𝛼−𝑞−2𝑉) is con inuous on
(𝑡𝑘,𝑡𝑘+1](𝑘=0,1) o e e y (𝑈,𝑉)∈𝑅2;
(ii) (𝑈,𝑉) → 𝑄(𝑡,𝑡𝛼−2𝑈,𝑡𝛼−𝑞−2𝑉)is con inuous on 𝑅2
o e e y 𝑡∈(0,1);
(iii) o each 𝑟>0 he e exis s a cons an 𝐵𝑟>0such ha
|𝑄(𝑡,𝑡𝛼−2𝑈,𝑡𝛼−𝑞−2𝑉)|≤𝐵𝑟,𝑡∈(0,1),|𝑈|,|𝑉|≤𝑟.
Lemma 5 ( he Le ay-Schaude nonlinea al e na i e [23]).
Le 𝑋be a Banach space and 𝑇:𝑋→𝑋be a comple ely
con inuous ope a o . Suppose Ωis a nonemp y open subse o 𝑋
cen e ed a ze o. Then ei he he e exis s 𝑥∈𝜕Ωand 𝜆∈(0,1)
such ha 𝑥=𝜆𝑇𝑥o he e exis s 𝑥∈Ωsuch ha 𝑥=𝑇𝑥.
Le he gamma and be a unc ions Γ(𝛼)and B(𝑝,𝑞)be
de ined by
Γ(𝛼)=∫+∞
0𝑥𝛼−1𝑒−𝑥𝑑𝑥,
B(𝑝,𝑞)=∫1
0𝑥𝑝−1(1−𝑥)𝑞−1𝑑𝑥,
‖𝑚‖1=∫1
0|𝑚(𝑠)|𝑑𝑠 o 𝑚∈𝐿1(0,1).
(11)
Choose
𝑋
=
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
𝑥|(𝑡𝑘,𝑡𝑘+1]∈𝐶0(𝑡𝑘,𝑡𝑘+1](𝑘=0,1),
𝐷𝑞
0+𝑥|(𝑡𝑘,𝑡𝑘+1]∈𝐶0(𝑡𝑘,𝑡𝑘+1](𝑘=0,1),
𝑥:(0,1]󳨀→ 𝑅 he e exis he limi s
lim
𝑡→𝑡+
𝑘𝑡2−𝛼𝑥(𝑡),
lim
𝑡→𝑡+
𝑘𝑡2+𝑞−𝛼𝐷𝑞
0+𝑥(𝑡)
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
,
𝑌
=
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
𝑦|(𝑡𝑘,𝑡𝑘+1]∈𝐶0(𝑡𝑘,𝑡𝑘+1](𝑘=0,1),
𝐷𝑝
0+𝑥|(𝑡𝑘,𝑡𝑘+1]∈𝐶0(𝑡𝑘,𝑡𝑘+1](𝑘=0,1),
𝑦:(0,1]󳨀→ 𝑅 he e exis he limi s
lim
𝑡→𝑡+
𝑘𝑡2−𝛽𝑦(𝑡),
lim
𝑡→𝑡+
𝑘𝑡2+𝑝−𝛽𝐷𝑝
0+𝑦(𝑡)
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
}
.
(12)
Fo 𝑥∈𝑋, de ine he no m by
‖𝑥‖=‖𝑥‖𝑋
=max {sup
𝑡∈(0,1)𝑡2−𝛼 |𝑥(𝑡)|,sup
𝑡∈(0,1)𝑡2+𝑞−𝛼 󵄨󵄨󵄨󵄨󵄨𝐷𝑞
0+𝑥(𝑡)󵄨󵄨󵄨󵄨󵄨}. (13)
I is easy o show ha 𝑋is a eal Banach space. Fo 𝑦∈𝑌,
de ine he no m by
󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩=󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩𝑌
=max {sup
𝑡∈(0,1)𝑡2−𝛽 󵄨󵄨󵄨󵄨𝑦(𝑡)󵄨󵄨󵄨󵄨,sup
𝑡∈(0,1)𝑡2+𝑝−𝛽 󵄨󵄨󵄨󵄨󵄨𝐷𝑝
0+𝑦(𝑡)󵄨󵄨󵄨󵄨󵄨}. (14)
I is easy o show ha 𝑌is a eal Banach space. Thus, (𝑋×
𝑌,||⋅||)is a Banach space wi h he no m de ined by ||(𝑥,𝑦)||=
max{||𝑥||𝑋,||𝑦||𝑌} o (𝑥,𝑦)∈𝑋×𝑌.
In his pape , we suppose he ollowing:
(A) 𝜙sa is ies ha he e exis cons an s 𝐿1>0,𝑘>−1,
𝛿∈(𝑞−𝛼,0]such ha 𝛼+2𝛿−𝑞>0,𝛼+𝑘+𝛿−𝑞≥0,
and |𝜙(𝑡)|≤𝐿1𝑡𝑘(1−𝑡)𝛿 o all 𝑡∈(0,1);𝜓sa is ies
ha he e exis cons an s 𝐿2>0,𝑙>−1,𝜃∈(𝑝−𝛽,0]
such ha 𝛽+2𝜃−𝑝>0,𝛽+𝑙+𝜃−𝑝≥0,and
|𝜓(𝑡)|≤𝐿2𝑡𝑙(1−𝑡)𝜃 o all 𝑡∈(0,1).
(B) 𝑓,𝐺,𝑀,𝐼,𝐼1a e 𝛽-Ca a heodo y unc ions and 𝑔,𝐻,
𝑁,𝐽,𝐽1a e 𝛼-Ca a heodo y unc ions.
Rema k 6. Suppose ha 𝑓is a 𝛽-Ca a heodo y unc ion. Fo
example, 𝛼=7/4,𝑞=1/8,choose𝑘=−1/2,𝛿=−3/4
and 𝜙(𝑡) = 𝑡𝑘(1−𝑡)𝛿, hen𝑘>−1,𝛿 ∈ (−𝛼,0]such ha
𝛼+2𝛿−𝑞>0,𝛼+𝑘+𝛿−𝑞≥0,and|𝜙(𝑡)|≤𝑡𝑘(1−𝑡)𝛿 o all
𝑡∈(0,1).I iseasy osee ha 𝜙is singula a 𝑡=0and 𝑡=1.
4Ma hema ical P oblems in Enginee ing
Lemma 7. Suppose ha 𝑦∈𝑌, and (a)–(e), (A)-(B) hold.
Then 𝑥∈𝑋is a solu ion o
𝐷𝛼
0+𝑥(𝑡)=𝜙(𝑡)𝑓(𝑡,𝑦(𝑡),𝐷𝑝
0+𝑦(𝑡)), 𝑡∈(0,1),𝑡=𝑡1,
lim
𝑡→0𝑡2−𝛼𝑥(𝑡)=∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠,
𝑥(1)=∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠,
Δ𝑥(𝑡1)=𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)),
Δ𝐷𝑞
0+𝑥(𝑡1)=𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)), (15)
i and only i 𝑥∈𝑋sa is ies he in eg al equa ion
𝑥(𝑡)=
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
∫𝑡
0(𝑡−𝑠)𝛼−1
Γ(𝛼)𝜙(𝑢)𝑓(𝑢,𝑦(𝑢),𝐷𝑝
0+𝑦(𝑢))𝑑𝑢
−𝑡𝛼−1
Γ(𝛼)
×∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−2 ∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−1 ∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−1
Π
×( Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1−Γ(𝛼−1)
Γ(𝛼−𝑞−2)𝑡𝛼−𝑞−2
1)
×𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
+𝑡𝛼−1 (𝑡𝛼−2
1−𝑡𝛼−1
1)
Π
×𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)), 𝑡∈(0,𝑡1],
∫𝑡
0(𝑡−𝑠)𝛼−1
Γ(𝛼)𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
−𝑡𝛼−1
Γ(𝛼)
×∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+(𝑡𝛼−2 −𝑡𝛼−1)
×∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−1 ∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−1 −𝑡𝛼−2
ΠΓ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1
×𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
+𝑡𝛼−2 −𝑡𝛼−1
Π𝑡𝛼−1
1𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)),
𝑡∈(𝑡1,1],
(16)
whe e
Π=( Γ(𝛼−1)
Γ(𝛼−𝑞−1)−Γ(𝛼)
Γ(𝛼−𝑞))𝑡2𝛼−𝑞−3
1.(17)
P oo . I 𝑦∈𝑌is a solu ion o BVP (15), hen
󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩=max {sup
𝑡∈(0,1)𝑡2−𝛽 󵄨󵄨󵄨󵄨𝑦(𝑡)󵄨󵄨󵄨󵄨,sup
𝑡∈(0,1)𝑡2+𝑝−𝛽 󵄨󵄨󵄨󵄨󵄨𝐷𝑝
0+𝑦(𝑡)󵄨󵄨󵄨󵄨󵄨}
=𝑟<+∞, (18)
and 𝑥sa is ies all equa ions in (31)F om(B),𝑓is a 𝛽-
Ca a heodo y unc ion, hen he e exis s 𝐴𝑟>0such ha
󵄨󵄨󵄨󵄨󵄨𝑓(𝑡,𝑦(𝑡),𝐷𝑝
0+𝑦(𝑡))󵄨󵄨󵄨󵄨󵄨
=󵄨󵄨󵄨󵄨󵄨𝑓(𝑡,𝑡𝛽−2𝑡2−𝛽𝑦(𝑡),𝑡𝛽−𝑝−2𝑡2+𝑝−𝛽𝐷𝑝
0+𝑦(𝑡))󵄨󵄨󵄨󵄨󵄨≤𝐴𝑟.
(19)
Simila ly we ge ha he e exis cons an s 𝐴󸀠
𝑟,𝐴󸀠󸀠
𝑟,𝐵󸀠
𝑟,𝐵󸀠󸀠
𝑟>0
such ha 󵄨󵄨󵄨󵄨󵄨𝐺(𝑡,𝑦(𝑡),𝐷𝑝
0+𝑦(𝑡))󵄨󵄨󵄨󵄨󵄨≤𝐴󸀠
𝑟,
󵄨󵄨󵄨󵄨󵄨𝑀(𝑡,𝑦(𝑡),𝐷𝑝
0+𝑦(𝑡))󵄨󵄨󵄨󵄨󵄨≤𝐴󸀠󸀠
𝑟,
𝑡∈(0,1),
󵄨󵄨󵄨󵄨󵄨𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))󵄨󵄨󵄨󵄨󵄨≤𝐵󸀠
𝑟,
󵄨󵄨󵄨󵄨󵄨𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))󵄨󵄨󵄨󵄨󵄨≤𝐵󸀠󸀠
𝑟.
(20)
I ollows om (15) ha , o 𝑡∈(𝑡𝑘,𝑡𝑘+1](𝑘=0,1), he e
exis cons an s 𝑐𝑘,𝑑𝑘∈𝑅such ha
𝑥(𝑡)=1
Γ(𝛼)∫𝑡
0(𝑡−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑐𝑘𝑡𝛼−1 +𝑑𝑘𝑡𝛼−2,𝑡∈(𝑡
𝑘,𝑡𝑘+1],𝑘=0,1. (21)
F om lim𝑡→0𝑡2−𝛼𝑥(𝑡) = ∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠,we
ge
𝑑0=∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠. (22)
F om 𝑥(1)=∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠,wege
1
Γ(𝛼)∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠+𝑐1+𝑑1
=∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠. (23)
F om Δ𝑥(𝑡1)=𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)),wege
(𝑐1−𝑐0)𝑡𝛼−1
1+(𝑑1−𝑑0)𝑡𝛼−2
1=𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)).
(24)
Ma hema ical P oblems in Enginee ing 5
F om Δ𝐷𝑞
0+𝑥(𝑡1)=𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)),wege
(𝑐1−𝑐0)Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1+(𝑑1−𝑑0)Γ(𝛼−1)
Γ(𝛼−𝑞−2)𝑡𝛼−𝑞−2
1
=𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)). (25)
I ollows ha
𝑐1−𝑐0=( Γ(𝛼−1)
Γ(𝛼−𝑞−2)𝑡𝛼−𝑞−2
1𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
−𝑡𝛼−2
1𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)))×(Π)−1,
𝑑1−𝑑0=(𝑡
𝛼−1
1𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
−Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)))
×(Π)−1.(26)
Then
𝑑1=(𝑡
𝛼−1
1𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
−Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)))×(Π)−1
+∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠. (27)
So
𝑐1=∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
−1
Γ(𝛼)∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
−(𝑡𝛼−1
1𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
−Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)))×(Π)−1
−∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠,
𝑐0=∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
−1
Γ(𝛼)∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
−(𝑡𝛼−1
1𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
−Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)))×(Π)−1
−∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
−( Γ(𝛼−1)
Γ(𝛼−𝑞−2)𝑡𝛼−𝑞−2
1𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
−𝑡𝛼−2
1𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)))×(Π)−1.
(28)
Hence, o 𝑡∈(0,𝑡1],weha e
𝑥(𝑡)=∫𝑡
0(𝑡−𝑠)𝛼−1
Γ(𝛼)𝜙(𝑢)𝑓(𝑢,𝑦(𝑢),𝐷𝑝
0+𝑦(𝑢))𝑑𝑢
−𝑡𝛼−1
Γ(𝛼)∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−2 ∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−1 ∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−1
Π(Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1−Γ(𝛼−1)
Γ(𝛼−𝑞−2)𝑡𝛼−𝑞−2
1)
×𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
+𝑡𝛼−1 (𝑡𝛼−2
1−𝑡𝛼−1
1)
Π𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)). (29)
And o 𝑡∈(𝑡1,1],weha e
𝑥(𝑡)=∫𝑡
0(𝑡−𝑠)𝛼−1
Γ(𝛼)𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
−𝑡𝛼−1
Γ(𝛼)∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+(𝑡𝛼−2 −𝑡𝛼−1)∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−1 ∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−1 −𝑡𝛼−2
ΠΓ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1
×𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
+𝑡𝛼−2 −𝑡𝛼−1
Π𝑡𝛼−1
1𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)).
(30)
Hence, 𝑥∈𝑋sa is ies (16).
On he o he hand, i 𝑦∈𝑌and 𝑥∈𝑋is a solu ion o (16),
hen we can p o e ha 𝑥∈𝑋is a solu ion o BVP (6)-(7). The
p oo is comple ed.

6Ma hema ical P oblems in Enginee ing
Lemma 8. Suppose ha 𝑥∈𝑋, and (a)–(e), (A)-(B) hold.
Then 𝑦∈𝑌is a solu ion o
𝐷𝛽
0+𝑦(𝑡)=𝜓(𝑡)𝑔(𝑡,𝑥(𝑡),𝐷𝑞
0+𝑥(𝑡)), 𝑡∈(0,1),𝑡=𝑡1,
lim
𝑡→0𝑡2−𝛽𝑦(𝑡)=∫1
0
V(𝑠)𝐻(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠,
𝑦(1)=∫1
0𝑛(𝑠)𝑁(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠,
Δ𝑦(𝑡1)=𝐽(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1)),
Δ𝐷𝑝
0+𝑦(𝑡1)=𝐽1(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1)), (31)
i and only i 𝑦∈𝑌sa is ies he in eg al equa ion
𝑦(𝑡)=
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
∫𝑡
0(𝑡−𝑠)𝛽−1
Γ(𝛽) 𝜓(𝑢)𝑔(𝑢,𝑥(𝑢),𝐷𝑞
0+𝑥(𝑢))𝑑𝑢
−𝑡𝛽−1
Γ(𝛽)
×∫1
0(1−𝑠)𝛽−1𝜓(𝑠)𝑔(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
+𝑡𝛽−2
×∫1
0
V(𝑠)𝐻(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛽−1
×∫1
0𝑛(𝑠)𝑁(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
+𝑡𝛽−1
Ξ
×( Γ(𝛽)
Γ(𝛽−𝑝)𝑡𝛽−𝑝−1
1−Γ(𝛽−1)
Γ(𝛽−𝑝−2)𝑡𝛽−𝑝−2
1)
×𝐽(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1))
+𝑡𝛽−1 (𝑡𝛽−2
1−𝑡𝛽−1
1)
Ξ
×𝐽1(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1)), 𝑡∈(0,𝑡1],
∫𝑡
0(𝑡−𝑠)𝛽−1
Γ(𝛽) 𝜓(𝑠)𝑔(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
−𝑡𝛽−1
Γ(𝛽)
×∫1
0(1−𝑠)𝛽−1𝜓(𝑠)𝑔(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
+(𝑡𝛽−2 −𝑡𝛽−1)
×∫1
0
V(𝑠)𝐻(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛽−1
×∫1
0𝑛(𝑠)𝑁(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
+𝑡𝛽−1 −𝑡𝛽−2
ΞΓ(𝛽)
Γ(𝛽−𝑝)𝑡𝛽−𝑝−1
1
×𝐽(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1))
+𝑡𝛽−2 −𝑡𝛽−1
Ξ𝑡𝛽−1
1
×𝐽1(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1)), 𝑡∈(𝑡1,1], (32)
whe e
Ξ=( Γ(𝛽−1)
Γ(𝛽−𝑝−1)−Γ(𝛽)
Γ(𝛽−𝑝))𝑡2𝛽−𝑝−3
1.(33)
P oo . The p oo is simila o ha o he p oo o Lemma 7
and is omi ed.
Now, we de ine he ope a o 𝑇on 𝑋×𝑌by 𝑇(𝑥,𝑦)(𝑡)=
((𝑇1𝑦)(𝑡),(𝑇2𝑥)(𝑡))wi h
(𝑇1𝑦)(𝑡)
=
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
∫𝑡
0(𝑡−𝑠)𝛼−1
Γ(𝛼)𝜙(𝑢)𝑓(𝑢,𝑦(𝑢),𝐷𝑝
0+𝑦(𝑢))𝑑𝑢
−𝑡𝛼−1
Γ(𝛼)∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−2 ∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−1 ∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−1
Π(Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1−Γ(𝛼−1)
Γ(𝛼−𝑞−2)𝑡𝛼−𝑞−2
1)
×𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
+𝑡𝛼−1 (𝑡𝛼−2
1−𝑡𝛼−1
1)
Π
×𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)), 𝑡∈(0,𝑡1],
∫𝑡
0(𝑡−𝑠)𝛼−1
Γ(𝛼)𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
−𝑡𝛼−1
Γ(𝛼)∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+(𝑡𝛼−2 −𝑡𝛼−1)∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−1 ∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−1 −𝑡𝛼−2
ΠΓ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
+𝑡𝛼−2 −𝑡𝛼−1
Π𝑡𝛼−1
1𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)),
𝑡∈(𝑡1,1], (34)
Ma hema ical P oblems in Enginee ing 7
(𝑇2𝑥)(𝑡)
=
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
∫𝑡
0(𝑡−𝑠)𝛽−1
Γ(𝛽) 𝜓(𝑢)𝑔(𝑢,𝑥(𝑢),𝐷𝑞
0+𝑥(𝑢))𝑑𝑢
−𝑡𝛽−1
Γ(𝛽)∫1
0(1−𝑠)𝛽−1𝜓(𝑠)𝑔(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
+𝑡𝛽−2 ∫1
0
V(𝑠)𝐻(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛽−1 ∫1
0𝑛(𝑠)𝑁(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
+𝑡𝛽−1
Ξ(Γ(𝛽)
Γ(𝛽−𝑝)𝑡𝛽−𝑝−1
1−Γ(𝛽−1)
Γ(𝛽−𝑝−2)𝑡𝛽−𝑝−2
1)
×𝐽(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1))
+𝑡𝛽−1 (𝑡𝛽−2
1−𝑡𝛽−1
1)
Ξ𝐽1(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1)),
𝑡∈(0,𝑡1],
∫𝑡
0(𝑡−𝑠)𝛽−1
Γ(𝛽) 𝜓(𝑠)𝑔(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
−𝑡𝛽−1
Γ(𝛽)∫1
0(1−𝑠)𝛽−1𝜓(𝑠)𝑔(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
+(𝑡𝛽−2 −𝑡𝛽−1)∫1
0
V(𝑠)𝐻(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛽−1 ∫1
0𝑛(𝑠)𝑁(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
+𝑡𝛽−1 −𝑡𝛽−2
ΞΓ(𝛽)
Γ(𝛽−𝑝)𝑡𝛽−𝑝−1
1
×𝐽(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1))
+𝑡𝛽−2 −𝑡𝛽−1
Ξ𝑡𝛽−1
1𝐽1(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1)),
𝑡∈(𝑡1,1]. (35)
Rema k 9. By Lemmas 7and 8,(𝑥,𝑦)∈𝑋×𝑌is a solu ion
o BVP (6)-(7)i andonlyi (𝑥,𝑦)∈𝑋×𝑌is a ixed poin o
he ope a o 𝑇.
Lemma 10. Suppose ha (a)–(e) and (A)-(B) hold. Then 𝑇:
𝑋×𝑌→𝑋×𝑌is well de ined and is comple ely con inuous.
P oo . The p oo is e y long, so we lis he s eps. Fi s , we
p o e ha 𝑇is well de ined; second, we p o e ha 𝑇is
con inuous, and, inally, we p o e ha 𝑇is compac . So 𝑇is
comple ely con inuous. Thus, he p oo is di ided in o h ee
s eps.
S ep 1. P o e ha 𝑇:𝑋×𝑌→𝑋×𝑌is well de ined.
Fo (𝑥,𝑦)∈𝑋×𝑌,weha e||(𝑥,𝑦)||=𝑟>0.Then
max {sup
𝑡∈(0,1)𝑡2−𝛼 |𝑥(𝑡)|,sup
𝑡∈(0,1)𝑡2+𝑞−𝛼 󵄨󵄨󵄨󵄨󵄨𝐷𝑞
0+𝑥(𝑡)󵄨󵄨󵄨󵄨󵄨}≤𝑟<+∞,
max {sup
𝑡∈(0,1)𝑡2−𝛽 󵄨󵄨󵄨󵄨𝑦(𝑡)󵄨󵄨󵄨󵄨,sup
𝑡∈(0,1)𝑡2+𝑝−𝛽 󵄨󵄨󵄨󵄨󵄨𝐷𝑝
0+𝑦(𝑡)󵄨󵄨󵄨󵄨󵄨}≤𝑟<+∞.
(36)
F om (B), 𝑓,𝐺,𝑀,𝐼,𝐼1a e 𝛽-Ca a heodo y unc ions, hen
he e exis cons an s 𝐴𝑟>0such ha
󵄨󵄨󵄨󵄨󵄨𝑓(𝑡,𝑦(𝑡),𝐷𝑝
0+𝑦(𝑡))󵄨󵄨󵄨󵄨󵄨≤𝐴𝑟,𝑡∈
(0,1),
󵄨󵄨󵄨󵄨󵄨𝐺(𝑡,𝑦(𝑡),𝐷𝑝
0+𝑦(𝑡))󵄨󵄨󵄨󵄨󵄨≤𝐴𝑟,𝑡∈
(0,1),
󵄨󵄨󵄨󵄨󵄨𝑀(𝑡,𝑦(𝑡),𝐷𝑝
0+𝑦(𝑡))󵄨󵄨󵄨󵄨󵄨≤𝐴𝑟,𝑡∈
(0,1),
󵄨󵄨󵄨󵄨󵄨𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))󵄨󵄨󵄨󵄨󵄨≤𝐴𝑟,𝑡∈
(0,1),
󵄨󵄨󵄨󵄨󵄨𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))󵄨󵄨󵄨󵄨󵄨≤𝐴𝑟,𝑡∈
(0,1).
(37)
Hence,
󵄨󵄨󵄨󵄨󵄨󵄨󵄨󵄨󵄨∫𝑡
0(𝑡−𝑠)𝛼−1
Γ(𝛼)𝜙(𝑢)𝑓(𝑢,𝑦(𝑢),𝐷𝑝
0+𝑦(𝑢))𝑑𝑢󵄨󵄨󵄨󵄨󵄨󵄨󵄨󵄨󵄨
≤∫𝑡
0(𝑡−𝑠)𝛼−1
Γ(𝛼)󵄨󵄨󵄨󵄨󵄨𝜙(𝑢)𝑓(𝑢,𝑦(𝑢),𝐷𝑝
0+𝑦(𝑢))󵄨󵄨󵄨󵄨󵄨𝑑𝑢
≤𝐴𝑟𝐿1
B(𝛼+𝛿,𝑘+1)
Γ(𝛼)<∞.
(38)
F om (34), (37), and (38), we see ha (𝑇1𝑦)(𝑡)is de ined on
(0,1],con inuouson(0,𝑡1]and (𝑡1,1], espec i ely.Onesees
ha
lim
𝑡→0𝑡2−𝛼 (𝑇1𝑦)(𝑡)
=lim
𝑡→0[𝑡2−𝛼 ∫𝑡
0(𝑡−𝑠)𝛼−1
Γ(𝛼)𝜙(𝑢)𝑓(𝑢,𝑦(𝑢),𝐷𝑝
0+𝑦(𝑢))𝑑𝑢
−𝑡
Γ(𝛼)∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡
Π(Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1−Γ(𝛼−1)
Γ(𝛼−𝑞−2)𝑡𝛼−𝑞−2
1)
×𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
+𝑡(𝑡𝛼−2
1−𝑡𝛼−1
1)
Π𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))]
=∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠, (39)
and he eexi s helimi lim
𝑡→𝑡+
1(𝑇1𝑦)(𝑡).
8Ma hema ical P oblems in Enginee ing
On he o he hand, we ha e
𝐷𝑞
0+(𝑇1𝑦)(𝑡)
=
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
∫𝑡
0(𝑡−𝑠)𝛼−𝑞−1
Γ(𝛼−𝑞) 𝜙(𝑢)𝑓(𝑢,𝑦(𝑢),𝐷𝑝
0+𝑦(𝑢))𝑑𝑢
−𝑡𝛼−𝑞−1
Γ(𝛼−𝑞)
×∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−𝑞−2 Γ(𝛼−1)
Γ(𝛼−𝑞−1)
×∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−𝑞−1 Γ(𝛼)
Γ(𝛼−𝑞)
×∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−𝑞−1
ΠΓ(𝛼)
Γ(𝛼−𝑞)
×( Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1−Γ(𝛼−1)
Γ(𝛼−𝑞−2)𝑡𝛼−𝑞−2
1)
×𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
+Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1 (𝑡𝛼−2
1−𝑡𝛼−1
1)
Π
×𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)), 𝑡∈(0,𝑡1],
∫𝑡
0(𝑡−𝑠)𝛼−𝑞−1
Γ(𝛼−𝑞) 𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
−𝑡𝛼−𝑞−1
Γ(𝛼−𝑞)
×∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+(𝑡𝛼−𝑞−2 Γ(𝛼−1)
Γ(𝛼−𝑞−1)−𝑡𝛼−𝑞−1 Γ(𝛼)
Γ(𝛼−𝑞))
×∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛼−𝑞−1 Γ(𝛼)
Γ(𝛼−𝑞)∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+1
Π(𝑡𝛼−𝑞−1 Γ(𝛼)
Γ(𝛼−𝑞)−𝑡𝛼−𝑞−2 Γ(𝛼−1)
Γ(𝛼−𝑞−1))
×Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
+1
Π(𝑡𝛼−𝑞−2 Γ(𝛼−1)
Γ(𝛼−𝑞−1)−𝑡𝛼−𝑞−1 Γ(𝛼)
Γ(𝛼−𝑞))
×𝑡𝛼−1
1𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1)), 𝑡∈(𝑡1,1],
𝐷𝑝
0+(𝑇2𝑥)(𝑡)
=
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
{
∫𝑡
0(𝑡−𝑠)𝛽−𝑝−1
Γ(𝛽−𝑝)𝜓(𝑢)𝑔(𝑢,𝑥(𝑢),𝐷𝑞
0+𝑥(𝑢))𝑑𝑢
−𝑡𝛽−𝑝−1
Γ(𝛽−𝑝)
×∫1
0(1−𝑠)𝛽−1𝜓(𝑠)𝑔(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
+𝑡𝛽−𝑝−2 Γ(𝛽−1)
Γ(𝛽−𝑝−1)
×∫1
0
V(𝑠)𝐻(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛽−𝑝−1 Γ(𝛽)
Γ(𝛽−𝑝)
×∫1
0𝑛(𝑠)𝑁(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
+𝑡𝛽−𝑝−1
ΞΓ(𝛽)
Γ(𝛽−𝑝)
×( Γ(𝛽)
Γ(𝛽−𝑝)𝑡𝛽−𝑝−1
1−Γ(𝛽−1)
Γ(𝛽−𝑝−2)𝑡𝛽−𝑝−2
1)
×𝐽(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1))
+𝑡𝛽−𝑝−1 (𝑡𝛽−2
1−𝑡𝛽−1
1)
ΞΓ(𝛽)
Γ(𝛽−𝑝)
×𝐽1(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1)), 𝑡∈(0,𝑡1],
∫𝑡
0(𝑡−𝑠)𝛽−𝑝−1
Γ(𝛽−𝑝)𝜓(𝑠)𝑔(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
−𝑡𝛽−𝑝−1
Γ(𝛽) Γ(𝛽)
Γ(𝛽−𝑝)
×∫1
0(1−𝑠)𝛽−1𝜓(𝑠)𝑔(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
+(𝑡𝛽−𝑝−2 Γ(𝛽−1)
Γ(𝛽−𝑝−1)−𝑡𝛽−𝑝−1 Γ(𝛽)
Γ(𝛽−𝑝))
×∫1
0
V(𝑠)𝐻(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡𝛽−𝑝−1 Γ(𝛽)
Γ(𝛽−𝑝)∫1
0𝑛(𝑠)𝑁(𝑠,𝑥(𝑠),𝐷𝑞
0+𝑥(𝑠))𝑑𝑠
+1
Ξ(𝑡𝛽−𝑝−1 Γ(𝛽)
Γ(𝛽−𝑝)−𝑡𝛽−𝑝−2 Γ(𝛽−1)
Γ(𝛽−𝑝−1))
×Γ(𝛽)
Γ(𝛽−𝑝)𝑡𝛽−𝑝−1
1𝐽(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1))
+1
Ξ(𝑡𝛽−𝑝−2 Γ(𝛽−1)
Γ(𝛽−𝑝−1)−𝑡𝛽−𝑝−1 Γ(𝛽)
Γ(𝛽−𝑝))
×𝑡𝛽−1
1𝐽1(𝑡1,𝑥(𝑡1),𝐷𝑞
0+𝑥(𝑡1)), 𝑡∈(𝑡1,1]. (40)
Ma hema ical P oblems in Enginee ing 9
I is easy o see ha
󵄨󵄨󵄨󵄨󵄨󵄨󵄨󵄨󵄨∫𝑡
0(𝑡−𝑠)𝛼−𝑞−1
Γ(𝛼−𝑞)𝜙(𝑢)𝑓(𝑢,𝑦(𝑢),𝐷𝑝
0+𝑦(𝑢))𝑑𝑢󵄨󵄨󵄨󵄨󵄨󵄨󵄨󵄨󵄨
≤𝐴𝑟𝐿1
B(𝛼+𝛿−𝑞,𝑘+1)
Γ(𝛼−𝑞) <∞. (41)
F om (37)and(41), we see ha 𝐷𝑞
0+(𝑇1𝑦)(𝑡)is de ined on
(0,1],con inuouson(0,𝑡1]and (𝑡1,1], espec i ely.Onesees
ha
lim
𝑡→0𝑡2+𝑞−𝛼𝐷𝑞
0+(𝑇1𝑦)(𝑡)
=lim
𝑡→0[𝑡2+𝑞−𝛼
×∫𝑡
0(𝑡−𝑠)𝛼−𝑞−1
Γ(𝛼−𝑞)𝜙(𝑢)𝑓(𝑢,𝑦(𝑢),𝐷𝑝
0+𝑦(𝑢))𝑑𝑢
−𝑡
Γ(𝛼−𝑞)
×∫1
0(1−𝑠)𝛼−1𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+Γ(𝛼−1)
Γ(𝛼−𝑞−1)∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡 Γ(𝛼)
Γ(𝛼−𝑞)∫1
0𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠
+𝑡
ΠΓ(𝛼)
Γ(𝛼−𝑞)
×( Γ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1−Γ(𝛼−1)
Γ(𝛼−𝑞−2)𝑡𝛼−𝑞−2
1)
×𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))
+Γ(𝛼)
Γ(𝛼−𝑞)𝑡(𝑡𝛼−2
1−𝑡𝛼−1
1)
Π
×𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))]
=Γ(𝛼−1)
Γ(𝛼−𝑞−1)∫1
0𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))𝑑𝑠,
(42)
and he e exi s he limi lim𝑡→𝑡+
1𝐷𝑞
0+(𝑇1𝑦)(𝑡).
F om he abo e discussion, we ha e (𝑇1𝑦)∈𝑋.Simila ly,
we can show ha (𝑇2𝑥)∈𝑌.Hence,((𝑇1𝑦),(𝑇2𝑥))∈𝑋×𝑌.
Then 𝑇:𝑋×𝑌→𝑋×𝑌is well de ined.
S ep 2. We p o e ha 𝑇is con inuous. Le (𝑥𝑛,𝑦𝑛)∈𝑋×
𝑌wi h (𝑥𝑛,𝑦𝑛)→(𝑥
0,𝑦0)as 𝑛→∞.Wewillshow ha
𝑇(𝑥𝑛,𝑦𝑛)→𝑇(𝑥
0,𝑦0)as 𝑛→∞, ha is,p o e ha 𝑇1𝑦𝑛→
𝑇1𝑦0and 𝑇2𝑥𝑛→𝑇
2𝑥0as 𝑛→∞.
In ac , we ha e 𝑟>0such ha ||(𝑥𝑛,𝑦𝑛)||=𝑟>0.Then
max {sup
𝑡∈(0,1)𝑡2−𝛼 󵄨󵄨󵄨󵄨𝑥𝑛(𝑡)󵄨󵄨󵄨󵄨,sup
𝑡∈(0,1)𝑡2+𝑞−𝛼 󵄨󵄨󵄨󵄨󵄨𝐷𝑞
0+𝑥𝑛(𝑡)󵄨󵄨󵄨󵄨󵄨}
≤𝑟<+∞, 𝑛=0,1,2,...,
max {sup
𝑡∈(0,1)𝑡2−𝛽 󵄨󵄨󵄨󵄨𝑦𝑛(𝑡)󵄨󵄨󵄨󵄨,sup
𝑡∈(0,1)𝑡2+𝑝−𝛽 󵄨󵄨󵄨󵄨󵄨𝐷𝑝
0+𝑦𝑛(𝑡)󵄨󵄨󵄨󵄨󵄨}
≤𝑟<+∞, 𝑛=0,1,2,....
(43)
F om (B), 𝑓,𝐺,𝑀,𝐼,𝐼1a e 𝛽-Ca a heodo y unc ions,
hen he e exis cons an s 𝐴𝑟>0such ha
󵄨󵄨󵄨󵄨󵄨𝑓(𝑡,𝑦𝑛(𝑡),𝐷𝑝
0+𝑦𝑛(𝑡))󵄨󵄨󵄨󵄨󵄨≤𝐴𝑟,
𝑡∈(0,1), 𝑛=0,1,2,...,
󵄨󵄨󵄨󵄨󵄨𝐺(𝑡,𝑦𝑛(𝑡),𝐷𝑝
0+𝑦𝑛(𝑡))󵄨󵄨󵄨󵄨󵄨≤𝐴𝑟,
𝑡∈(0,1), 𝑛=0,1,2,...,
󵄨󵄨󵄨󵄨󵄨𝑀(𝑡,𝑦𝑛(𝑡),𝐷𝑝
0+𝑦𝑛(𝑡))󵄨󵄨󵄨󵄨󵄨≤𝐴𝑟,
𝑡∈(0,1), 𝑛=0,1,2,...,
󵄨󵄨󵄨󵄨󵄨𝐼(𝑡1,𝑦𝑛(𝑡1),𝐷𝑝
0+𝑦𝑛(𝑡1))󵄨󵄨󵄨󵄨󵄨≤𝐴𝑟,
𝑡∈(0,1), 𝑛=0,1,2,...,
󵄨󵄨󵄨󵄨󵄨𝐼1(𝑡1,𝑦𝑛(𝑡1),𝐷𝑝
0+𝑦𝑛(𝑡1))󵄨󵄨󵄨󵄨󵄨≤𝐴𝑟,
𝑡∈(0,1), 𝑛=0,1,2,...,
sup
𝑡∈(0,1)𝑡2−𝛼 󵄨󵄨󵄨󵄨𝑥𝑛(𝑡)−𝑥0(𝑡)󵄨󵄨󵄨󵄨󳨀→ 0,
sup
𝑡∈(0,1)𝑡2−𝛽 󵄨󵄨󵄨󵄨𝑦𝑛(𝑡)−𝑦0(𝑡)󵄨󵄨󵄨󵄨,
sup
𝑡∈(0,1)𝑡2+𝑞−𝛼 󵄨󵄨󵄨󵄨󵄨𝐷𝑞
0+𝑥𝑛(𝑡)−𝐷𝑞
0+𝑥0(𝑡)󵄨󵄨󵄨󵄨󵄨󳨀→ 0,
sup
𝑡∈(0,1)𝑡2+𝑝−𝛽 󵄨󵄨󵄨󵄨󵄨𝐷𝑝
0+𝑦𝑛(𝑡)−𝐷𝑝
0+𝑦0(𝑡)󵄨󵄨󵄨󵄨󵄨󳨀→ 0,
(44)
16 Ma hema ical P oblems in Enginee ing
+Γ(𝛽)
Γ(𝛽−𝑝)‖𝑛‖1[𝐵𝑁+𝐴𝑁]
+1
ΞΓ(𝛽)
Γ(𝛽−𝑝)
×󵄨󵄨󵄨󵄨󵄨󵄨󵄨󵄨󵄨Γ(𝛽)
Γ(𝛽−𝑝)𝑡𝛽−𝑝−1
1−Γ(𝛽−1)
Γ(𝛽−𝑝−2)𝑡𝛽−𝑝−2
1󵄨󵄨󵄨󵄨󵄨󵄨󵄨󵄨󵄨[𝐵𝐽+𝐴𝐽]
+Γ(𝛽)
Γ(𝛽−𝑝)󵄨󵄨󵄨󵄨󵄨󵄨𝑡𝛽−2
1−𝑡𝛽−1
1󵄨󵄨󵄨󵄨󵄨󵄨
Ξ[𝐵1,𝐽 +𝐴1,𝐽],
Λ1=𝐿2
B(𝛽+𝜃,𝑙+1)
Γ(𝛽) 𝐶𝑔+𝐿2B(𝛽+𝜃,𝑙+1)
Γ(𝛽) 𝐶𝑔
+‖V‖1𝐶𝐻+1
ΞΓ(𝛽)
Γ(𝛽−𝑝)𝑡𝛽−𝑝−1
1𝐶𝐽+1
Ξ𝑡𝛽−1
1𝐶1,𝐽,
Λ2=𝐿2
B(𝛽+𝜃,𝑙+1)
Γ(𝛽) [𝐵𝑔+𝐴𝑔]
+𝐿2B(𝛽+𝜃,𝑙+1)
Γ(𝛽) [𝐵𝑔+𝐴𝑔]+‖V‖1[𝐵𝐻+𝐴𝐻]
+1
ΞΓ(𝛽)
Γ(𝛽−𝑝)𝑡𝛽−𝑝−1
1[𝐵𝐽+𝐴𝐽]+1
Ξ𝑡𝛽−1
1[𝐵1,𝐽 +𝐴1,𝐽],
Λ3=𝐿2
B(𝛽+𝜃−𝑝,𝑙+1)
Γ(𝛽−𝑝) 𝐶𝑔
+𝐿2
Γ(𝛽−𝑝)B(𝛽+𝜃,𝑙+1)𝐶𝑔
+( Γ(𝛽−1)
Γ(𝛽−𝑝−1)+Γ(𝛽)
Γ(𝛽−𝑝))‖V‖1𝐶𝐻
+Γ(𝛽)
Γ(𝛽−𝑝)‖𝑛‖1𝐶𝑁
+1
Ξ(Γ(𝛽)
Γ(𝛽−𝑝)+Γ(𝛽−1)
Γ(𝛽−𝑝−1))Γ(𝛽)
Γ(𝛽−𝑝)𝑡𝛽−𝑝−1
1𝐶𝐽
+1
Ξ(Γ(𝛽−1)
Γ(𝛽−𝑝−1)+Γ(𝛽)
Γ(𝛽−𝑝))𝑡𝛽−1
1𝐶1,𝐽,
Λ4=𝐿2
B(𝛽+𝜃−𝑝,𝑙+1)
Γ(𝛽−𝑝) [𝐵𝑔+𝐴𝑔]
+𝐿2
Γ(𝛽−𝑝)B(𝛽+𝜃,𝑙+1)[𝐵𝑔+𝐴𝑔]
+( Γ(𝛽−1)
Γ(𝛽−𝑝−1)+Γ(𝛽)
Γ(𝛽−𝑝))‖V‖1[𝐵𝐻+𝐴𝐻]
+Γ(𝛽)
Γ(𝛽−𝑝)‖𝑛‖1[𝐵𝑁+𝐴𝑁]
+1
Ξ(Γ(𝛽)
Γ(𝛽−𝑝)+Γ(𝛽−1)
Γ(𝛽−𝑝−1))
×Γ(𝛽)
Γ(𝛽−𝑝)𝑡𝛽−𝑝−1
1[𝐵𝐽+𝐴𝐽]
+1
Ξ(Γ(𝛽−1)
Γ(𝛽−𝑝−1)+Γ(𝛽)
Γ(𝛽−𝑝))𝑡𝛽−1
1[𝐵1,𝐽 +𝐴1,𝐽].
(81)
P oo . To apply Lemma 5, we should de ine an open bounded
subse Ωo 𝑋×𝑌cen e ed a ze o such ha assump ions in
Lemma 5hold.
Le Ω1={(𝑥,𝑦)∈𝑋×𝑌: (𝑥,𝑦)=𝜆𝑇(𝑥,𝑦) o some
𝜆∈(0,1)}.Wep o e ha Ω1is bounded. Fo (𝑥,𝑦)∈Ω1,we
ge (𝑥,𝑦)=𝜆𝑇(𝑥,𝑦).I ollows ha 𝑥=𝜆𝑇1𝑦and 𝑦=𝜆𝑇2𝑥.
Fo 𝑡∈(0,𝑡
1],weob ain𝑡2−𝛼|𝑥(𝑡)| ≤ 𝑡2−𝛼|(𝑇1𝑦)(𝑡)| ≤
Θ1+Θ2Φ−1(||𝑦||).
Fo 𝑡∈(𝑡1,1],
𝑡2−𝛼 |𝑥(𝑡)|
≤𝑡2−𝛼 ∫𝑡
0(𝑡−𝑠)𝛼−1
Γ(𝛼)󵄨󵄨󵄨󵄨󵄨𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))󵄨󵄨󵄨󵄨󵄨𝑑𝑠
+𝑡
Γ(𝛼)∫1
0(1−𝑠)𝛼−1 󵄨󵄨󵄨󵄨󵄨𝜙(𝑠)𝑓(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))󵄨󵄨󵄨󵄨󵄨𝑑𝑠
+(1−𝑡)∫1
0󵄨󵄨󵄨󵄨󵄨𝑢(𝑠)𝐺(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))󵄨󵄨󵄨󵄨󵄨𝑑𝑠
+𝑡∫1
0󵄨󵄨󵄨󵄨󵄨𝑚(𝑠)𝑀(𝑠,𝑦(𝑠),𝐷𝑝
0+𝑦(𝑠))󵄨󵄨󵄨󵄨󵄨𝑑𝑠
+1−𝑡
ΠΓ(𝛼)
Γ(𝛼−𝑞)𝑡𝛼−𝑞−1
1󵄨󵄨󵄨󵄨󵄨𝐼(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))󵄨󵄨󵄨󵄨󵄨
+1−𝑡
Π𝑡𝛼−1
1󵄨󵄨󵄨󵄨󵄨𝐼1(𝑡1,𝑦(𝑡1),𝐷𝑝
0+𝑦(𝑡1))󵄨󵄨󵄨󵄨󵄨
≤Σ1+Σ2Φ−1 (󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩). (82)
I ollows ha
sup
𝑡∈(0,1)𝑡2−𝛼 |𝑥(𝑡)|≤max {Θ1,Σ1}+max {Θ2,Σ2}Φ−1 (󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩).
(83)
Simila ly, we ha e o 𝑡∈(0,𝑡1] ha
𝑡𝑞+2−𝛼 󵄨󵄨󵄨󵄨󵄨𝐷𝑞
0+𝑥(𝑡)󵄨󵄨󵄨󵄨󵄨≤Θ3+Θ4Φ−1 (󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩)(84)
and o 𝑡∈(0,𝑡1]
𝑡𝑞+2−𝛼 󵄨󵄨󵄨󵄨󵄨𝐷𝑞
0+𝑥(𝑡)󵄨󵄨󵄨󵄨󵄨≤Σ3+Σ4Φ−1 (󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩). (85)
I ollows ha
sup
𝑡∈(0,1)𝑡2+𝑞−𝛼 󵄨󵄨󵄨󵄨󵄨𝐷𝑞
0+𝑥(𝑡)󵄨󵄨󵄨󵄨󵄨
≤max {Θ3,Σ3}+max {Θ4,Σ4}Φ−1 (󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩). (86)

Ma hema ical P oblems in Enginee ing 17
Hence,
‖𝑥‖≤max {Θ1,Σ1,Θ3,Σ3}
+max {Θ2,Σ2,Θ4,Σ4}Φ−1 (󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩). (87)
Simila o heabo ediscussionwecanp o e ha
󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩≤max {Υ1,Λ1,Υ3,Λ3}+max {Υ2,Λ2,Υ4,Λ4}Φ(‖𝑥‖).
(88)
Case 1. Conside (max{Θ2,Σ2,Θ4,Σ4}](2max{Υ2,Λ2,Υ4,
Λ4})<1).
Wi hou losso gene ali y,suppose ha
‖𝑥‖≥Φ−1 (max {Υ1,Λ1,Υ3,Λ3}
max {Υ2,Λ2,Υ4,Λ4}). (89)
Then use Rema k 13, and he p e ious inequali ies o ge
‖𝑥‖≤max {Θ1,Σ1,Θ3,Σ3}
+max {Θ2,Σ2,Θ4,Σ4}](2max {Υ2,Λ2,Υ4,Λ4})‖𝑥‖.
(90)
I ollows ha he e exis s a cons an 𝑊>0such ha ||𝑥||≤
𝑊.Thus
‖𝑥‖≤max {𝑊,Φ−1 (max {Υ1,Λ1,Υ3,Λ3}
max {Υ2,Λ2,Υ4,Λ4})}. (91)
Then
󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩≤max {Υ1,Λ1,Υ3,Λ3}
+max {Υ2,Λ2,Υ4,Λ4}Φ
×(max {𝑊,Φ−1 (max {Υ1,Λ1,Υ3,Λ3}
max {Υ2,Λ2,Υ4,Λ4})}).
(92)
I ollows ha Ω1is bounded.
Case 2. Conside ((max{Υ2,Λ2,Υ4,Λ4}/𝑤((2max{Θ2,Σ2,
Θ4,Σ4})−1)) <1).
Wi hou loss o gene ali y, suppose ha
󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩≥Φ(max {Θ1,Σ1,Θ3,Σ3}
max {Θ2,Σ2,Θ4,Σ4}). (93)
Then using Rema k 12 and he p e ious inequali ies, we ge
󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩≤max {Υ1,Λ1,Υ3,Λ3}
+max {Υ2,Λ2,Υ4,Λ4}
𝑤((2max {Θ2,Σ2,Θ4,Σ4})−1)󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩.(94)
I ollows ha he e exis s a cons an 𝑊>0such ha ||𝑦||≤
𝑊.Wege
󵄩󵄩󵄩󵄩𝑦󵄩󵄩󵄩󵄩≤max {𝑊,Φ(max {Θ1,Σ1,Θ3,Σ3}
max {Θ2,Σ2,Θ4,Σ4})}. (95)
Then
‖𝑥‖≤max {Θ1,Σ1,Θ3,Σ3}
+max {Θ2,Σ2,Θ4,Σ4}Φ−1
×(max {𝑊,Φ(max {Θ1,Σ1,Θ3,Σ3}
max {Θ2,Σ2,Θ4,Σ4})}).
(96)
I ollows ha Ω1is bounded.
To apply Lemma 5,le Ωbe a nonemp y open bounded
subse o 𝑋such ha Ω⊃Ω1cen e ed a ze o.
I is easy o see om Lemma 8 ha 𝑇is a comple ely con-
inuous ope a o . One can see ha
(𝑥,𝑦) =𝜆𝑇(𝑥,𝑦) ∀(𝑥,𝑦)∈𝜕Ω,𝜆∈(0,1).(97)
Thus, om Lemma 5,(𝑥,𝑦)=𝑇(𝑥,𝑦)has a leas one solu ion
(𝑥,𝑦)∈Ω.So(𝑥,𝑦)is a pai o solu ions o BVP (3)andBVP
(6). The p oo o Theo em 14 is comple e.
4. Two Examples
To illus a e he use ulness o ou main esul , we p esen wo
examples ha Theo em 14 can eadily apply.
Example 15. Conside he ollowing impulsi e bounda y
alue p oblem:
𝐷8/5
0+𝑥(𝑡)=𝑡−1/5(1−𝑡)−1
×(𝑐+𝑏𝑡6/5[𝑦(𝑡)]3+𝑎𝑡9/5[𝐷1/5
0+𝑦(𝑡)]3),
𝑡∈(0,1),𝑡=1
2,
𝐷9/5
0+𝑦(𝑡)
=𝑡−1/5(1−𝑡)−1
×(𝑐0+𝑏0𝑡1/15[𝑥(𝑡)]1/3 +𝑎0𝑡2/15[𝐷1/5
0+𝑥(𝑡)]1/3),
𝑡∈(0,1),𝑡=𝑡1,
lim
𝑡→0𝑡2/5𝑥(𝑡)=𝐺, lim
𝑡→0𝑡1/5𝑦(𝑡)=𝐻,
𝑥(1)=𝑀, 𝑦(1)=𝑁,
Δ𝑥(1
2)=𝑐𝐼,Δ𝑦(
1
2)=𝑐𝐽,
Δ𝐷1
0+𝑥(1
2)=𝑐1,𝐼,Δ𝐷
1
0+𝑦(1
2)=𝑐1,𝐽,(98)
whe e 𝑐,𝑏,𝑎,𝑐0,𝑏0,𝑎0,𝐺0,𝐻0,𝑀0,𝑁0,𝐶𝐼,𝐶𝐽,𝐶1,𝐼,𝐶1,𝐽
a e cons an s.
Co esponding o BVP (1), we ha e
(a) 𝛼=8/5,𝛽=9/5,𝑝=𝑞=1/5,
(b) 𝜙(𝑡)=𝜓(𝑡)=𝑡−1/5(1−𝑡)−1/5,𝑓(𝑡,𝑈,𝑉)=𝑐+𝑏𝑡6/5𝑈3+
𝑎𝑡9/5𝑉3and 𝑔(𝑡,𝑈,𝑉)=𝑐0+𝑏0𝑡1/15𝑈1/3 +𝑎0𝑡2/15𝑉1/3
de ined on (0,1)×𝑅2,
18 Ma hema ical P oblems in Enginee ing
(c) 𝑢(𝑡)=V(𝑡)=𝑚(𝑡)=𝑛(𝑡)≡1,𝐺(𝑡,𝑈,𝑉)=𝐺0,𝐻(𝑡,
𝑈,𝑉)=𝐻0,𝑀(𝑡,𝑈,𝑉)=𝑀0,𝑁(𝑡,𝑈,𝑉)=𝑁0,
(d) 0=𝑡0<𝑡1=(1/2)<𝑡2=1,
(e) 𝐼(𝑡,𝑈,𝑉)=𝑐𝐼,𝐼1(𝑡,𝑈,𝑉)=𝑐1,𝐼,𝐽(𝑡,𝑈,𝑉)=𝑐𝐽,𝐽1(𝑡,
𝑈,𝑉)=𝑐1,𝐽.
I is easy o show ha
(A) 𝜙sa is ies 𝛼+2𝛿−𝑞>0,𝛼+𝑘+𝛿−𝑞≥0,and
|𝜙(𝑡)|≤𝐿1𝑡𝑘(1−𝑡)𝛿 o all 𝑡∈(0,1)wi h 𝐿1=1and
𝑘=−(1/5)=𝛿;
𝜓sa is ies 𝜂+2𝜃−𝑝>0,𝛽+𝑙+𝜃−𝑝≥0,and
|𝜓(𝑡)|≤𝐿2𝑡𝑙(1−𝑡)𝜃 o all 𝑡∈(0,1)wi h 𝐿2=1and
𝑙=−(1/5)=𝜃;
(B) 𝑓,𝐺,𝑀,𝐼,𝐼1a e 𝛽-Ca a heodo y unc ions and 𝑔,𝐻,
𝑁,𝐽,𝐽1a e 𝛼-Ca a heodo y unc ions.
Fu he mo e, we ha e Φ−1(𝑥)=𝑥3and Φ(𝑥)=𝑥1/3 wi h
𝑤(𝑥)=𝑥1/3 and ](𝑥)=𝑥3.I iseasy osee ha
(i) he inequali ies
󵄨󵄨󵄨󵄨󵄨𝑓(𝑡,𝑡𝛼−2𝑈,𝑡𝛼−𝑞−2𝑉)󵄨󵄨󵄨󵄨󵄨≤𝐶𝑓+𝐵𝑓Φ−1 (|𝑈|)+𝐴𝑓Φ−1 (|𝑉|),
󵄨󵄨󵄨󵄨󵄨𝐺(𝑡,𝑡𝛼−2𝑈,𝑡𝛼−𝑞−2𝑉)󵄨󵄨󵄨󵄨󵄨≤𝐶𝐺+𝐵𝐺Φ−1 (|𝑈|)+𝐴𝐺Φ−1 (|𝑉|),
󵄨󵄨󵄨󵄨󵄨𝑀(𝑡,𝑡𝛼−2𝑈,𝑡𝛼−𝑞−2𝑉)󵄨󵄨󵄨󵄨󵄨
≤𝐶𝑀+𝐵𝑀Φ−1 (|𝑈|)+𝐴𝑀Φ−1 (󵄨󵄨󵄨󵄨󵄨Φ−1 (|𝑈|)󵄨󵄨󵄨󵄨󵄨)(99)
hold o all (𝑈,𝑉)∈𝑅2,𝑡∈(0,1]wi h 𝐶𝑓=|𝑐|,𝐵𝑓=
|𝑏|,𝐴𝑓=|𝑎|,𝐶𝐺=|𝐺0|,𝐵𝐺=0,𝐴𝐺=0and 𝐶𝑀=
|𝑀0|,𝐵𝑀=0,𝐴𝑀=0;
(ii) he inequali ies
󵄨󵄨󵄨󵄨󵄨𝑔(𝑡,𝑡𝛽−2𝑈,𝑡𝛽−𝑝−2𝑉)󵄨󵄨󵄨󵄨󵄨≤𝐶𝑔+𝐵𝑔Φ(𝑈)+𝐴𝑔Φ(𝑉),
󵄨󵄨󵄨󵄨󵄨𝐻(𝑡,𝑡𝛽−2𝑈,𝑡𝛽−𝑝−2𝑉)󵄨󵄨󵄨󵄨󵄨≤𝐶𝐻+𝐵𝐻Φ(𝑈)+𝐴𝐻Φ(𝑉),
󵄨󵄨󵄨󵄨󵄨𝑁(𝑡,𝑡𝛽−2𝑈,𝑡𝛽−𝑝−2𝑉)󵄨󵄨󵄨󵄨󵄨≤𝐶𝑁+𝐵𝑁Φ(𝑈)+𝐴𝑁Φ(𝑉)
(100)
hold o all (𝑈,𝑉) ∈ 𝑅2,𝑡 ∈ (0,1]wi h 𝐶𝑔=|𝑐
0|,
𝐵𝑔=|𝑏
0|,𝐴𝑔=|𝑎
0|,𝐶𝐻=|𝐻
0|,𝐵𝐻=𝐴
𝐻=0,
𝐶𝑁=|𝑁0|,𝐵𝑁=𝐴𝑁=0;
(iii) he inequali ies
󵄨󵄨󵄨󵄨󵄨𝐼(𝑡1,𝑡𝛼−2
1𝑈,𝑡𝛼−𝑞−2
1𝑉)󵄨󵄨󵄨󵄨󵄨≤𝐶𝐼+𝐵𝐼Φ−1 (|𝑈|)+𝐴𝐼Φ−1 (|𝑉|),
󵄨󵄨󵄨󵄨󵄨𝐼1(𝑡1,𝑡𝛼−2
1𝑈,𝑡𝛼−𝑞−2
1𝑉)󵄨󵄨󵄨󵄨󵄨
≤𝐶1,𝐼 +𝐵1,𝐼Φ−1 (|𝑈|)+𝐴1,𝐼Φ−1 (|𝑉|)(101)
hold o all (𝑈,𝑉)∈𝑅2wi h 𝐶𝐼=|𝑐
𝐼|,𝐵𝐼=𝐴𝐼=0,
𝐶1,𝐼 =|𝑐1,𝐼|,𝐵1,𝐼 =𝐴1,𝐼 =0;
(i ) he inequali ies
󵄨󵄨󵄨󵄨󵄨󵄨𝐽(𝑡1,𝑡𝛽−2
1𝑈,𝑡𝛽−𝑝−2
1𝑉)󵄨󵄨󵄨󵄨󵄨󵄨≤𝐶𝐽+𝐵𝐽Φ(𝑈)+𝐴𝐽Φ(𝑉),
󵄨󵄨󵄨󵄨󵄨󵄨𝐽1(𝑡1,𝑡𝛽−2
1𝑈,𝑡𝛽−𝑝−2
1𝑉)󵄨󵄨󵄨󵄨󵄨󵄨≤𝐶1,𝐽 +𝐵1,𝐽Φ(𝑈)+𝐴1,𝐽Φ(𝑉)
(102)
hold o all (𝑈,𝑉)∈𝑅2wi h 𝐶𝐽=|𝑐
𝐽|,𝐵𝐽=𝐴𝐽=0,
𝐶1,𝐽 =|𝑐1,𝐽|,𝐵1,𝐽 =𝐴1,𝐽 =0.
By di ec compu a ion, we know ha
Θ2=2B(7/5,4/5)
Γ(8/5)[|𝑏|+|𝑎|],
Σ2=2B(7/5,4/5)
Γ(8/5)[|𝑏|+|𝑎|],
Θ4=(B(6/5,4/5)
Γ(7/5)+B(7/5,4/5)
Γ(7/5))[|𝑏|+|𝑎|],
Σ4=(B(6/5,4/5)
Γ(7/5)+B(7/5,4/5)
Γ(7/5))[|𝑏|+|𝑎|],
Υ2=2B(8/5,4/5)
Γ(9/5)[󵄨󵄨󵄨󵄨𝑏0󵄨󵄨󵄨󵄨+󵄨󵄨󵄨󵄨𝑎0󵄨󵄨󵄨󵄨],
Υ4=(B(7/5,4/5)
Γ(8/5)+B(8/5,4/5)
Γ(8/5))[󵄨󵄨󵄨󵄨𝑏0󵄨󵄨󵄨󵄨+󵄨󵄨󵄨󵄨𝑎0󵄨󵄨󵄨󵄨],
Λ2=2B(8/5,4/5)
Γ(9/5)[󵄨󵄨󵄨󵄨𝑏0󵄨󵄨󵄨󵄨+󵄨󵄨󵄨󵄨𝑎0󵄨󵄨󵄨󵄨],
Λ4=(B(7/5,4/5)
Γ(8/5)+B(8/5,4/5)
Γ(8/5))[󵄨󵄨󵄨󵄨𝑏0󵄨󵄨󵄨󵄨+󵄨󵄨󵄨󵄨𝑎0󵄨󵄨󵄨󵄨].
(103)
Then Theo em 14 implies ha he exis ence o a leas one
solu ion i
max {2B(8/5,4/5)
Γ(9/5),B(7/5,4/5)
Γ(8/5)+B(8/5,4/5)
Γ(8/5)}
×(max {2B(7/5,4/5)
Γ(8/5) ,B(6/5,4/5)
Γ(7/5) +B(7/5,4/5)
Γ(7/5) })1/3
×[󵄨󵄨󵄨󵄨𝑏0󵄨󵄨󵄨󵄨+󵄨󵄨󵄨󵄨𝑎0󵄨󵄨󵄨󵄨][|𝑏|+|𝑎|]1/3 <1
3
√2.(104)
Example 16. Conside he ollowing bounda y alue p oblem
wi hou impulse e ec s:
𝐷7/4
0+𝑥(𝑡)=𝑡−1/4(1−𝑡)−1/4
×(𝐶+𝐵𝑡3/4[𝑦(𝑡)]3+𝐴𝑡15/4[𝐷1
0+𝑦(𝑡)]3),
𝑡∈(0,1),
Ma hema ical P oblems in Enginee ing 19
𝐷5/4
0+𝑦(𝑡)
=𝑡−1/8(1−𝑡)−1/8
×(𝐶0+𝐵0𝑡1/4[𝑥(𝑡)]1/3 +𝐴0𝑡7/12[𝐷1/4
0+𝑥(𝑡)]1/3),
𝑡∈(0,1),
lim
𝑡→0𝑡1/4𝑥(𝑡)=0, lim
𝑡→0𝑡3/4𝑦(𝑡)=0,
𝑥(1)=0, 𝑦(1)=0, (105)
whe e 𝐶,𝐵,𝐴,𝐶0,𝐵0,and𝐴0a e cons an s.
Co esponding o BVP (1), we ha e
(a) 𝛼=7/4,𝛽=5/4,𝑝=1and 𝑞=1/4,
(b) 𝜙(𝑡) = 𝑡−1/4(1 − 𝑡)−1/4,𝜓(𝑡) = 𝑡−1/8(1 − 𝑡)−1/8,
𝑓,𝑔 de ined on (0,1) × 𝑅2,𝑓(𝑡,𝑈,𝑉) = 𝐶 +
𝐵𝑡1/12𝑈3+𝐴𝑡5/12𝑉3and 𝑔(𝑡,𝑈,𝑉)=𝐶0+𝐵0𝑡1/4𝑈1/3+
𝐴0𝑡7/12𝑉1/3,
(c) 𝑚(𝑡)=𝑛(𝑡)=𝑢(𝑡) = V(𝑡)≡0,𝐺(𝑡,𝑈,𝑉)=𝐻(𝑡,𝑈,
𝑉)=𝑀(𝑡,𝑈,𝑉)=𝑁(𝑡,𝑈,𝑉)≡0,
(d) he e exis s no impulse poin ,
(e) 𝐼(𝑡,𝑈,𝑉)=𝐼1(𝑡,𝑈,𝑉)=𝐽(𝑡,𝑈,𝑉)=𝐽1(𝑡,𝑈,𝑉)≡0.
I is easy o show ha
(A) 𝜙sa is ies 𝛼+2𝛿−𝑞>0,𝛼+𝑘+𝛿−𝑞>0,|𝜙(𝑡)|≤
𝐿1𝑡𝑘(1−𝑡)𝛿 o all 𝑡∈(0,1)wi h 𝐿1=1,𝑘=−(1/4)=
𝛿;
𝜓sa is ies 𝛽+2𝜃−𝑝>0,𝛽+𝑙+𝜃−𝑝≥0,and
|𝜓(𝑡)| ≤ 𝐿2𝑡𝑙(1−𝑡)𝜃 o all 𝑡 ∈ (0,1)wi h 𝐿2=1,
𝑙=−(1/8)=𝜃;
(B) 𝑓,𝐺,𝑀,𝐼,𝐼1a e 𝛽-Ca a heodo y unc ions and 𝑔,𝐻,
𝑁,𝐽,𝐽1a e 𝛼-Ca a heodo y unc ions.
Fu he mo e, Φ(𝑥)=𝑥1/3 and Φ−1(𝑥)=𝑥3,weha e𝑤(𝑥)=
𝑥1/3 and ](𝑥)=𝑥3,and
(i) he inequali ies
󵄨󵄨󵄨󵄨󵄨𝑓(𝑡,𝑡𝛼−2𝑈,𝑡𝛼−𝑞−2𝑉)󵄨󵄨󵄨󵄨󵄨≤𝐶𝑓+𝐵𝑓Φ−1 (|𝑈|)+𝐴𝑓Φ−1 (|𝑉|),
󵄨󵄨󵄨󵄨󵄨𝐺(𝑡,𝑡𝛼−2𝑈,𝑡𝛼−𝑞−2𝑉)󵄨󵄨󵄨󵄨󵄨≤𝐶𝐺+𝐵𝐺Φ−1 (|𝑈|)+𝐴𝐺Φ−1 (|𝑉|),
󵄨󵄨󵄨󵄨󵄨𝑀(𝑡,𝑡𝛼−2𝑈,𝑡𝛼−𝑞−2𝑉)󵄨󵄨󵄨󵄨󵄨
≤𝐶𝑀+𝐵𝑀Φ−1 (|𝑈|)+𝐴𝑀Φ−1 (󵄨󵄨󵄨󵄨󵄨Φ−1 (|𝑈|)󵄨󵄨󵄨󵄨󵄨)(106)
hold o all (𝑈,𝑉) ∈ 𝑅2,𝑡 ∈ (0,1)wi h 𝐶𝐺=𝐵
𝐺=
𝐴𝐺=𝐶𝑀=𝐵𝑀=𝐴𝑀=0,𝐶𝑓=|𝐶|,𝐵𝑓=|𝐵|and
𝐴𝑓=|𝐴|;
(ii) he inequali ies
󵄨󵄨󵄨󵄨󵄨𝑔(𝑡,𝑡𝛽−2𝑈,𝑡𝛽−𝑝−2𝑉)󵄨󵄨󵄨󵄨󵄨≤𝐶𝑔+𝐵𝑔Φ(𝑈)+𝐴𝑔Φ(𝑉),
󵄨󵄨󵄨󵄨󵄨𝐻(𝑡,𝑡𝛽−2𝑈,𝑡𝛽−𝑝−2𝑉)󵄨󵄨󵄨󵄨󵄨≤𝐶𝐻+𝐵𝐻Φ(𝑈)+𝐴𝐻Φ(𝑉),
󵄨󵄨󵄨󵄨󵄨𝑁(𝑡,𝑡𝛽−2𝑈,𝑡𝛽−𝑝−2𝑉)󵄨󵄨󵄨󵄨󵄨≤𝐶𝑁+𝐵𝑁Φ(𝑈)+𝐴𝑁Φ(𝑉)(107)
hold o all (𝑈,𝑉)∈𝑅2,𝑡 ∈(0,1)wi h 𝐶𝐻=𝐵𝐻=
𝐴𝐻=𝐶𝑁=𝐵𝑁=𝐴𝑁=0,𝐶𝑔=|𝐶0|,𝐵𝑔=|𝐵0|and
𝐴𝑔=|𝐴0|;
(iii) he inequali ies
󵄨󵄨󵄨󵄨󵄨𝐼(𝑡1,𝑡𝛼−2
1𝑈,𝑡𝛼−𝑞−2
1𝑉)󵄨󵄨󵄨󵄨󵄨
≤𝐶𝐼+𝐵𝐼Φ−1 (|𝑈|)+𝐴𝐼Φ−1 (|𝑉|),
󵄨󵄨󵄨󵄨󵄨𝐼1(𝑡1,𝑡𝛼−2
1𝑈,𝑡𝛼−𝑞−2
1𝑉)󵄨󵄨󵄨󵄨󵄨
≤𝐶1,𝐼 +𝐵1,𝐼Φ−1 (|𝑈|)+𝐴1,𝐼Φ−1 (|𝑉|)
(108)
hold o all (𝑈,𝑉)∈𝑅2wi h 𝐶𝐼=𝐵𝐼=𝐴𝐼=𝐶1,𝐼 =
𝐵1,𝐼 =𝐴1,𝐼 =0;
(i ) he e exis he nonnega i e numbe s 𝐴𝑖,𝑘,𝐵𝑖,𝑘,
𝐶𝑖,𝑘 (𝑖=1,2)such ha
󵄨󵄨󵄨󵄨󵄨󵄨𝐽(𝑡1,𝑡𝛽−2
1𝑈,𝑡𝛽−𝑝−2
1𝑉)󵄨󵄨󵄨󵄨󵄨󵄨≤𝐶𝐽+𝐵𝐽Φ(𝑈)+𝐴𝐽Φ(𝑉),
󵄨󵄨󵄨󵄨󵄨󵄨𝐽1(𝑡1,𝑡𝛽−2
1𝑈,𝑡𝛽−𝑝−2
1𝑉)󵄨󵄨󵄨󵄨󵄨󵄨≤𝐶1,𝐽 +𝐵1,𝐽Φ(𝑈)+𝐴1,𝐽Φ(𝑉)
(109)
hold o all (𝑈,𝑉)∈𝑅2wi h 𝐶𝐽=𝐵𝐽=𝐴𝐽=𝐶1,𝐽 =
𝐵1,𝐽 =𝐴1,𝐽 =0.
By di ec compu a ion, we know ha
Θ2=2B(3/2,3/4)
Γ(7/4)[|𝐵|+|𝐴|],
Σ2=2B(3/2,3/4)
Γ(7/4)[|𝐵|+|𝐴|],
Θ4=(B(5/4,3/4)
Γ(3/2)+B(3/2,3/4)
Γ(3/2))[|𝐵|+|𝐴|],
Σ4=(B(5/4,3/4)
Γ(3/2)+B(3/2,3/4)
Γ(3/2))[|𝐵|+|𝐴|],
Υ2=2B(9/8,7/8)
Γ(5/4)[󵄨󵄨󵄨󵄨𝐵0󵄨󵄨󵄨󵄨+󵄨󵄨󵄨󵄨𝐴0󵄨󵄨󵄨󵄨],
Υ4=(B(1/8,7/8)
Γ(𝛽−𝑝) +B(9/8,7/8)
Γ(1/4))[󵄨󵄨󵄨󵄨𝐵0󵄨󵄨󵄨󵄨+󵄨󵄨󵄨󵄨𝐴0󵄨󵄨󵄨󵄨],
Λ2=2B(9/8,7/8)
Γ(5/4)[󵄨󵄨󵄨󵄨𝐵0󵄨󵄨󵄨󵄨+󵄨󵄨󵄨󵄨𝐴0󵄨󵄨󵄨󵄨],
Λ4=(B(1/8,7/8)
Γ(1/4)+B(9/8,7/8)
Γ(1/4))[󵄨󵄨󵄨󵄨𝐵0󵄨󵄨󵄨󵄨+󵄨󵄨󵄨󵄨𝐴0󵄨󵄨󵄨󵄨].
(110)
20 Ma hema ical P oblems in Enginee ing
Then Theo em 14 implies he exis ence o a leas one
solu ion i
max {2B(3/2,3/4)
Γ(7/4),B(5/4,3/4)
Γ(3/2)+B(3/2,3/4)
Γ(3/2)}
×(max {2B(9/8,7/8)
Γ(5/4) ,B(1/8,7/8)
Γ(𝛽−𝑝) +B(9/8,7/8)
Γ(1/4) })3
×[󵄨󵄨󵄨󵄨𝐵0󵄨󵄨󵄨󵄨+󵄨󵄨󵄨󵄨𝐴0󵄨󵄨󵄨󵄨]3[|𝐵|+|𝐴|]<1
8.
(111)
Rema k 17. I is easy o see ha he p e ious bounda y alue
p oblems ha e a leas one solu ion o su icien ly small
|𝐵1|,|𝐵2|and |𝐴0|,|𝐵0|,|𝑎|,|𝑏|,|𝑎0|and |𝑏0|.Theycanno be
sol ed by he heo ems in [24,25].
Acknowledgmen s
This esea chispa iallysuppo edby heNa u alScience
Founda ion o Guangdong p o ince (no. S2011010001900)
and he Guangdong Highe Educa ion Founda ion o High-
Le el Talen s. This esea ch is pa ially suppo ed by Minis-
e io de Econom´
ıa y Compe i i idad and EC und FEDER,
P ojec no. MTM2010-15314, Spain.
Re e ences
[1] K. S. Mille and B. Ross, An In oduc ion o he F ac ional
CalculusandF ac ionalDi e en ialEqua ions,Wiley,NewYo k,
NY, USA, 1993.
[2] S.G.Samko,A.A.Kilbas,andO.I.Ma iche ,F ac ional In eg al
and De i a i e. Theo y and Applica ions, Go don and B each,
1993.
[3] A. A. Kilbas, H. M. S i as a a, and J. J. T ujillo, Theo y
and Applica ions o F ac ional Di e en ial Equa ions, ol.204
o No h-Holland Ma hema ics S udies, Else ie Science B.V.,
Ams e dam, The Ne he lands, 2006.
[4] B. Ahmad and J. J. Nie o, “An i-pe iodic ac ional bounda y
alue p oblems wi h nonlinea e m depending on lowe o de
de i a i e,” F ac ional Calculus and Applied Analysis, ol.15,no.
3, pp. 451–462, 2012.
[5] B.Ahmad,J.J.Nie o,A.Alsaedi,andM.El-Shahed,“As udyo
nonlinea Lange in equa ion in ol ing wo ac ional o de s in
di e en in e als,” Nonlinea Analysis: Real Wo ld Applica ions,
ol.13,no.2,pp.599–606,2012.
[6] I. Podlubny and N. Heymans, “Physical in e p e a ion o ini ial
condi ions o ac ional di e en ial equa ions wi h Riemann-
Liou ille ac ional de i a i es,” Rheologica Ac a, ol.45,no.5,
pp.765–771,2006.
[7] I. Podlubny, “Geome ic and physical in e p e a ion o ac-
ional in eg a ion and ac ional di e en ia ion,” F ac ional
Calculus and Applied Analysis, ol.5,no.4,pp.367–386,2002.
[8] A. Ca pin e i and F. Maina di, Eds., F ac als and F ac ional
Calculus in Con inuum Mechanics,CISMCou sesandLec u es,
In e na ional Cen e o Mechanical Sciences, no. 378, Sp inge ,
New Yo k, NY, USA, 1997.
[9] R. L. Magin, “F ac ional calculus in bioenginee ing, pa 1,”
C i ical Re iews in Biomedical Enginee ing, ol.32,no.1,pp.1–
104, 2004.
[10] R. L. Magin, “F ac ional calculus in bioenginee ing, pa 2,”
C i ical Re iews in Biomedical Enginee ing, ol.32,no.1,pp.105–
193, 2004.
[11] R. L. Magin, “F ac ional calculus in bioenginee ing, pa 3,”
C i ical Re iews in Biomedical Enginee ing, ol.32,no.3-4,pp.
195–377, 2004.
[12] X. Chen, L. Wei, J. Sui, and L. Zheng, “Sol ing he linea ime-
ac ional wa e equa ion by gene alized di e en ial ans o m
me hod,” Applied Mechanics and Ma e ials, ol.204–208,pp.
4476–4480, 2012.
[13] S. Li, B. Fang, T. Yang, Y. Zhang, L. Tan, and W. Huang,
“Dynamics o ib a ion isola ion sys em obeying ac ional
di e en ia ion,” Ai c a Enginee ing and Ae ospace Technology,
ol.84,no.2,pp.103–108,2012.
[14] G. S. P iya, P. P akash, J. J. Nie o, and Z. Kaya , “Highe o de
nume ical scheme o ac ional hea equa ion wi h Di ichle
and Neumann bounda y condi ions,” Nume ical Hea T ans e
B.Inp ess.
[15] J.Zhao,B.Tang,S.Kuma ,andY.Hou,“Theex ended ac ional
subequa ion me hod o nonlinea ac ional di e en ial equa-
ions,” Ma hema ical P oblems in Enginee ing, ol.2012,A icle
ID924956,11pages,2012.
[16] V. V. Lakshmikan ham, D. D. Ba˘
ıno , and P. S. Simeono , Theo y
o Impulsi e Di e en ial Equa ions, Wo ld Scien i ic, Singapo e,
1989.
[17] V. Ka i ha and M. Mallika A junan, “Con ollabili y o impul-
si e quasi-linea ac ional mixed Vol e a-F edholm- ype in e-
g odi e en ial equa ions in Banach spaces,” The Jou nal o
Nonlinea Science and I s Applica ions, ol.4,no.2,pp.152–169,
2011.
[18] B. Ahmad and S. Si asunda am, “Exis ence esul s o nonlinea
impulsi e hyb id bounda y alue p oblems in ol ing ac ional
di e en ial equa ions,” Nonlinea Analysis: Hyb id Sys ems, ol.
3, no. 3, pp. 251–258, 2009.
[19] B. Ahmad and S. Si asunda am, “Exis ence o solu ions o
impulsi e in eg al bounda y alue p oblems o ac ional
o de ,” Nonlinea Analysis: Hyb id Sys ems, ol.4,no.1,pp.134–
141, 2010.
[20] B. Ahmad and J. J. Nie o, “Exis ence o solu ions o impulsi e
an i-pe iodic bounda y alue p oblems o ac ional o de ,”
Taiwanese Jou nal o Ma hema ics, ol.15,no.3,pp.981–993,
2011.
[21] Y. Tian and Z. Bai, “Exis ence esul s o he h ee-poin impul-
si e bounda y alue p oblem in ol ing ac ional di e en ial
equa ions,” Compu e s & Ma hema ics wi h Applica ions, ol.59,
no. 8, pp. 2601–2609, 2010.
[22] R. P. Aga wal, M. Benchoh a, and S. Hamani, “A su ey on
exis ence esul s o bounda y alue p oblems o nonlinea ac-
ional di e en ial equa ions and inclusions,” Ac a Applicandae
Ma hema icae, ol.109,no.3,pp.973–1033,2010.
[23] J. Mawhin, Topological Deg ee Me hods in Nonlinea Bounda y
Value P oblems, ol.40o NSFCBMS Regional Con e ence Se ies
in Ma hema ics, Ame ican Ma hema ical Socie y, P o idence,
RI, USA, 1979.
[24] B. Ahmad and J. J. Nie o, “Exis ence esul s o a coupled
sys em o nonlinea ac ional di e en ial equa ions wi h h ee-
poin bounda y condi ions,” Compu e s & Ma hema ics wi h
Applica ions, ol.58,no.9,pp.1838–1843,2009.
Ma hema ical P oblems in Enginee ing 21
[25] X. Su, “Bounda y alue p oblem o a coupled sys em o non-
linea ac ional di e en ial equa ions,” Applied Ma hema ics
Le e s, ol.22,no.1,pp.64–69,2009.
[26] G. L. Ka akos as, “Posi i e solu ions o he Φ-Laplacian when
Φis a sup-mul iplica i e-like unc ion,” Elec onic Jou nal o
Di e en ial Equa ions, ol.2004,no.68,pp.1–12,2004.

Submi you manusc ip s a
h p://www.hindawi.com
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
Ma hema ics
Jou nal o
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
Ma hema ical P oblems
in Enginee ing
Hindawi Publishing Co po a ion
h p://www.hindawi.com
Di e en ial Equa ions
In e na ional Jou nal o
Volume 2014
Applied Ma hema ics
Jou nal o
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
P obabili y and S a is ics
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
Jou nal o
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
Ma hema ical Physics
Ad ances in
Complex Analysis
Jou nal o
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
Op imiza ion
Jou nal o
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
Combina o ics
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
In e na ional Jou nal o
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
Ope a ions Resea ch
Ad ances in
Jou nal o
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
Func ion Spaces
Abs ac and
Applied Analysis
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
In e na ional
Jou nal o
Ma hema ics and
Ma hema ical
Sciences
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
The Scien i ic
Wo ld Jou nal
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
Algeb a
Disc e e Dynamics in
Na u e and Socie y
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
Decision Sciences
Ad ances in
Disc e e Ma hema ics
Jou nal o
Hindawi Publishing Co po a ion
h p://www.hindawi.com
Volume 2014
Hindawi Publishing Co po a ion
h p://www.hindawi.com Volume 2014
S ochas ic Analysis
In e na ional Jou nal o