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On One Algorithm To Find a Solution to a Linear Two-Point Boundary Value Problem

Authors:
ISSN 1995-0802, Lobachevskii Journal of Mathematics, 2021, Vol. 42, No. 3, pp. 606–612. c
Pleiades Publishi ng, Ltd., 2021.
On One Algorithm To Find a Solution
to a Linear Two-Point Boundary Value Problem
S. M. Temesheva1*, D. S. Dzhumabaev2, and S. S. Kabdrakhova1**
(Submitted by T. K. Yuldashev)
1Department of Dierential Equations,
Institute of Mathematics and Mathematical Modeling, Al-Farabi Kazakh National University,
Almaty, Kazakhstan
2Department of Dierential Equations, Institute of Mathematics and Mathematical Modeling,
Almaty, Kazakhstan
Received June 14, 2020; revised July20, 2020; accepted July 31, 2020
AbstractA two-parameter family of algorithms for nding an approximate solution to a linear
two-point boundary value problem for a system of ordinary dierential equations is oered. The
convergence conditions for the algorithms are obtained. The necessary and sucient coecient
conditions for the well-posedness of considered problem are established.
DOI: 10.1134/S1995080221030173
Keywords and phrases: boundary value problem, system of ordinary dierential equations,
algorithms, parametrization method, necessary and sucient conditions.
1. INTRODUCTION
Consider a linear two-point boundary value problem
dx
dt =A(t)x+f(t),xRn,t(0,T),(1)
Bx(0) + Cx(T)=d, (2)
where A(t)and f(t)are continuous on [0,T],Band Care the given (n×n)matrices, dis a given n
vector, ||x|| =max
i=1:n|xi|,and||A(t)|| =max
i=1:n
n
j=1 |aij (t)|≤α,α=const.
Denote by C([0,T],Rn)the space of continuous functions x:[0,T]Rnwith the norm ||x||0=
max
t[0,T ]||x(t)||.
Solution to problem (1), (2) is a function x(t)C([0,T],Rn), continuously dierentiable on (0,T)
and satisfying the dierential equation (1) and boundary condition (2).
Boundary value problems for ordinary dierential equations are widely used in many application
areas [112]. To research and solve boundary value problems for ordinary dierential equations there
used various methods of qualitative theory of dierential equations and integral equations. The review
and bibliography can be found in [28, 10, 12]. Based on these methods, the conditions for the
solvability of boundary value problems were established, and the ways for nding the solutions were
suggested. Note that under some appropriate substitutions, the ordinary dierential equations of higher
orders lead to a system of ordinary dierential equations [2, 5, 10, 12]. The approximate and numerical
methods gain a particular importance for constructing the solutions to boundary value problems for
*E-mail: temeshevasvetlana@gmail.com
**E-mail: s_kabdrachova@mail.ru
606
ON ONE ALGORITHM TO FIND 607
equations and systems of ordinary dierential equations [9, 11, 13]. This article is focused on the
establishment of coecient criteria for the unique solvability of two-point boundary value problems for a
system of ordinary dierential equations and on the construction of a constructive method for nding an
approximate solution to problem (1), (2).
In [8], to investigate and solve a problem (1), (2) there is suggested a parametrization method.
Interval [0,T]in this method is divided into equal parts with step h>0:Nh =T(NN).Thenpa-
rameters λr,r=1:N, and new unknown functions ur(t),t[(r1)h, rh),r=1:N, are introduced,
and hereafter the initial problem is reduced to the equivalent problem with parameters. To nd a pair
system (λr,u
r(t)),r=1:N, the solution of latter problem, there is oered a two-parameter family of
algorithms, where h>0and the number of repeated integrals νused for the construction of matrix
Qν(h):RnN RnN are the numerical parameters of this family. Each algorithm’s step consists of two
items: a)nding of parameters λr,r=1:N, from the system of linear algebraic equations, which is
compiled on the initial data of problem (1), (2); b)nding of function ur(t), which is the solution of
Cauchy problem on interval [(r1)h, rh)at the given value of parameter λrfor all r=1:N.
Present article oers an other family of algorithms of parametrization method. Herein each algo-
rithm’s step also consists of two items. The dierence of oering algorithms is in item b),wherethe
unknown functions ur(t),t[(r1)h, rh),r=1:N, are to be computed by the recurrent formula.
The results are illustrated by an example, implemented in MathCAD software.
2. MODIFICATION OF ALGORITHM THE PARAMETRIZATION METHOD
Take some step h>0:Nh =T(NN) and make a partition of interval [0,T)according to this
step:
[0,T)=
N
r=1
[(r1)h, rh).
We will denote by C([0,T],h,RnN )the Banach space of function systems x[t]=x1(t),x
2(t),...,
xN(t)with the norm ||x[·]||1=max
r=1:Nsup
t[(r1)h,rh)||xr(t)||,where xr:[(r1)h, rh)Rnis continu-
ousandhasanite limit lim
trh0xr(t)for all r=1:N.
Let xr(t):xr(t)=x(t),t[(r1)h, rh),r=1:N, denote the restriction of function x(t)to the
r-th interval [(r1)h, rh)and reduce the problem (1), (2) to the equivalent multi-point boundary value
problem
dxr
dt =A(t)xr+f(t),t[(r1)h, rh),r=1:N, (3)
Bx1(0) + Clim
tNh0xN(t)=d, (4)
lim
tsh0xs(t)=xs+1(sh),s=1:(N1),(5)
where (5) are the conditions bonding the solution of problem (1), (2) at interior points of [0,T]-interval’s
partition.
Suppose that P(t)is a square matrix continuous on [(r1)h, rh)or a vector of dimension nand it
has a nite limit lim
trh0P(t),r=1:N. TakeanumericνNand denote by Eν,r(A(·),P(·),t)the sum
t
(r1)h
P(τ1)1+
t
(r1)h
A(τ1)
τ2
(r1)h
P(τ2)21+...
+
t
(r1)h
A(τ1)...
τν2
(r1)h
A(τν1)
τν1
(r1)h
P(τν)νν1...dτ
1,
LOBACHEVSKII JOURNAL OF MATHEMATICS Vol. 42 No. 3 2021
608 TEMESHEVA et al.
t[(r1)h, rh),r=1:N.
Sum Eν,r(A(·),P(·),t)is continuous on [(r1)h, rh)and has a nite limit
lim
trh0Eν,r(A(·),P(·),t)=Eν,r(A(·),P(·),rh)
for all νN,r=1:N. It is evident that E,r (A(·),P(·),t) = lim
ν→∞Eν,r(A(·),P(·),t)is a sum of
uniformly convergent series on [(r1)h, rh),and the sum is continuous on [(r1)h, rh)and has a
nite limit
lim
trh0E,r(A(·),P(·),t)=E,r(A(·),P(·),rh),r=1:N.
Let λrdenote the value of function xr(t)at point t=(r1)h. Making a replacement ur(t)=
xr(t)λr,r=1:Non [(r1)h, rh),we obtain a multi-point boundary value problem with parameters
dur
dt =A(t)(λr+ur)+f(t),t[(r1)h, rh),r=1:N, (6)
ur((r1)h)=0,r=1:N, (7)
1+N+Clim
tNh0uN(t)=d, (8)
λs+ lim
tsh0us(t)=λs+1,s=1:(N1).(9)
Pair λ,u
[t]with the elements λ=λ
1
2,...,λ
NRnN ,u[t]=u
1(t),u
2(t),...,u
N(t)
C([0,T],h,RnN )is a solution to problem (6)(9). Here the function u
r(t)isasolutiontoCauchy
problem (6), (7) with λr=λ
r,r=1:Nand, for λ
r,lim
trh0u
r(t),r=1:N, equalities (8), (9) hold.
Problems (1), (2) and (6)(9) are equivalent. If x(t)is a solution to problem (1), (2), then the
pair (λ,u
[t]) is a solution to problem (6)(9). Here λ=(λ
1
2,...,λ
N)RnN ,λ
r=x
r((r
1)h),u[t]=(u
1(t),u
2(t),...,u
N(t)),u
r(t)=x
r(t)x
r((r1)h),t[(r1)h, rh),andx
r(t)is a
restriction of function x(t)to [(r1)h, rh),r=1:N. Conversely, if the pair (
λ, u[t]) with components
λ=(
λ1,
λ2,...,
λN)RnN ,u[t]=(u1(t),u2(t),...,uN(t)) is a solution to problem (6)(9), then the
function x(t)dened by equalities
x(t)=
λr+ur(t),t[(r1)h, rh),r=1:N, and x(T)=
λN+ lim
tNh0uN(t)
is a solution to problem (1), (2). Problem with parameters diers from the boundary value problem
(3)(5) by the presence of initial conditions (7) for the new unknown functions.
For a xed value of the parameter λr,r=1:N, Cauchy problem (6), (7) is equivalent to the Volterra
integral equation [14] of second kind
ur(t)=
t
(r1)h
A(τ)(λr+ur(τ))+
t
(r1)h
f(τ)dτ, t [(r1)h, rh),r=1:N. (10)
Substituting the right-hand side of (10) instead of ur(τ)and repeating the process ν(νN)times, we
obtain the following presentment of function ur(t):
ur(t)=Dν,r(t)λr+Fν,r (t)+Gν,r(ur,t),t[(r1)h, rh),r=1:N, (11)
where Dν,r(t)=Eν,r (A(·),A(·),t),Fν,r (t)=Eν,r(A(·),f(·),t),and
Gν,r(ur,t)=
t
(r1)h
A(τ1)...
τν1
(r1)h
A(τν)ur(τν)ν...dτ
1,t[(r1)h, rh),r=1:N.
LOBACHEVSKII JOURNAL OF MATHEMATICS Vol. 42 No. 3 2021
ON ONE ALGORITHM TO FIND 609
Determine lim
trh0ur(t),r=1:Nfrom formula (11). Substituting the appropriate expressions into
(8), (9) pre-multiplying (8) by h>0:Nh =T, we obtain a system of linear algebraic equations with
respect to parameters:
Qν(h)λ=Fν(h)Gν(u, h)RnN,
where
Qν(h)=
hB O O ... O hC(I+Dν,N (Nh))
I+Dν,1(h)I O ... O O
OI+Dν,2(2h)I ... O O
... ... ... ... ... ...
O O O ... IO
O O O ... I +Dν,N 1((N1)h)I
,
I:RnRnis the identity matrix, O:RnRnis a zero matrix,
Fν(h)=hd +hCFν,N (Nh),F
ν,1(h),...,F
ν,N1((N1)h)RnN ,
Gν(u, h)=hCGν,N (uN,Nh),G
ν,1(u1,h),...,G
ν,N1(uN1,(N1)h)RnN .
Find (λ, u[t]), the solution to the multi-point boundary value problem with parameters (6)(9), where
λ=(λ1
2,...,λ
N)RnN ,u[t]=(u1(t),u
2(t),...,u
N(t)), according to the next algorithm. Suppose
that given ν,hthe matrix Qν(h):RnN RnN has an inverse one.
Step 0. a)Find the initial approximation on parameter λ(0) =(λ(0)
1
(0)
2,..., λ
(0)
N)RnN solving
the system of functions Qν(h)λ=Fν(h).
b)Determine the components of function system u(0)[t]=(u(0)
1(t),u
(0)
2(t),...,u
(0)
N(t)) according to
the formulas
u(0)
r(t)=Dν,r(t)λ(0)
r+Fν,r(t),t[(r1)h, rh),r=1:N.
Step 1. a)Find the next approximation on parameter λ(1) =(λ(1)
1
(1)
2,...,λ
(1)
N)RnN solving the
system of equations Qν(h)λ=Fν(h)Gν(u(0),h).
b)Determine the components of function system u(1)[t]=(u(1)
1(t),u
(1)
2(t),...,u
(1)
N(t)) according to
the formulas
u(1)
r(t)=Dν,r(t)λ(1)
r+Fν,r(t)+Gν,r(u(0)
r,t),t[(r1)h, rh),r=1:N.
And so on. Continuing this process, at the k-th step of algorithm we obtain the pair (λ(k),u
(k)[t]),
k=0,1,....
3. RESULTS
Theorem 1. Suppose that for some h>0:Nh =T(NN),νN, the matrix Qν(h):RnN
RnN is invertible and the following inequalities
||(Qν(h))1|| ≤ γν(h),q
ν(h)=(αh)ν
ν!
1+γν(h)max(1,h||C||)
ν
j=1
(αh)j
j!
<1
hold. Then at k→∞the sequence of pairs (λ(k),u
(k)[t]),k=0,1,...,dened by the algorithm
converges to (λ,u
[t]),a unique solution to the problem with parameters (6)(9), and the
estimates
||u[·]u(k)[·]||1qν(h)
1qν(h)||u(k)[·]u(k1)[·]||1,kN,
LOBACHEVSKII JOURNAL OF MATHEMATICS Vol. 42 No. 3 2021
610 TEMESHEVA et al.
||λλ(k)|| ≤ γν(h)
1qν(h)max(1,h||C||)(αh)ν
ν!||u(k)[·]u(k1)[·]||1,kN,
are true.
Denition 1. A problem (1), (2) is called well-posed if given any f(t)C([0,T],Rn),dRn
the problem has a unique solution x(t).
In light of equivalence of problems (1), (2) and (6)(9) the Theorem 1 leads to
Theorem 2. Given some h>0:Nh =T(NN),νNsuppose that the conditions of
Theorem 1 hold. Then the boundary value problem (1), (2) is uniquely solvable.
Next assertions demonstrate that the conditions of Theorem 2 are not only sucient, but necessary
as well for a unique solvability of problem (1), (2).
Theorem 3. If the boundary value problem (1), (2) is uniquely solvable, thengiven any h>0:
Nh =T(NN),χ(0,1] there exists ν=ν(h, χ)(νN)such that the matrix Qν(h):RnN RnN
is invertible, and the inequalities
||(Qν(h))1|| γν(h),(12)
qν(h)=(αh)ν
ν!1+γν(h)max(1,h||C||)
ν
j=1
(αh)j
j!(13)
hold.
Theorem 4. If the boundary value problem (1), (2) is uniquely solvable, then given any
ν(νN)(0,1] there exists a number
h=
h(ν, χ)>0such that for all h(0,
h]:Nh =T
(NN)the matrix Qν(h):RnN RnN is invertible and the inequalities (12), (13) hold.
4. EXAMPLE
Consider as an example the two-point boundary value problem for a system of two linear equations
of the rst order on [0,1]
dx1
dt =x2,
dx2
dt =t2x1+tx2t4+t32t2+t+2,
x1,x
2R1,(14)
x1(0) = 0,x
2(1) = 1.(15)
Solution to this problem is a vector function x(t)C([0,1],R2)with coordinates x
1(t)=t2t,
x
2(t)=2t1. For this problem, α=2 and at h=0.25,ν=3the matrix Qν(h)and vector Fν(h)
take the form
Q3(0.25) =
0.2500 0000000
0000000.2558 0.0700
1.0003 0.2527 100000
0.0053 1.0327 0 10000
001.0037 0.2611 10 0 0
000.0381 1.1041 0 10 0
00001.0113 0.2702 10
00000.1069 1.1845 0 1
,
F3(0.25) = (0.0000,0.0128,0.0652,0.5327,0.0686,0.5591,0.0650,0.5264),det Q3(0.25) =0.Since
||(Q3(0.25))1|| ≤ 13.6069,q
3(0.25) = 0.2039 <1,then, in accordance with Theorem 2, problem (14),
(15) is uniquely solvable.
LOBACHEVSKII JOURNAL OF MATHEMATICS Vol. 42 No. 3 2021
ON ONE ALGORITHM TO FIND 611
Solving the system of equations Q3(0.25)λ=F3(0.25) on the 0-step of algorithm, we nd λ(0)
R8and compute the components of function system u(0) [t]C([0,1],0.25,R8):
λ(0) =λ(0)
11
(0)
12
(0)
21
(0)
22
(0)
31
(0)
32
(0)
41
(0)
42
=(0.0000,0.9991,0.1873,0.4991,0.2497,0.0000,0.1872,0.5009),
u(0)[t]=u(0)
11 (t),u
(0)
12 (t),u
(0)
21 (t),u
(0)
22 (t),u
(0)
31 (t),u
(0)
32 (t),u
(0)
41 (t),u
(0)
42 (t):
u(0)
11 (t)=t2t+O(t),u
(0)
12 (t)=2t+O(t2),t[0,0.25),
u(0)
21 (t)=t2t+0.187271 + O(t),u
(0)
22 (t)=2t0.500029 + O(t2),t[0.25,0.5),
u(0)
31 (t)=t2t+0.249405 + O(t),u
(0)
32 (t)=2t10.000127 + O(t2),t[0.5,0.75),
u(0)
41 (t)=t2t+0.179727 + O(t),u
(0)
42 (t)=2t10.502316 + O(t2),t[0.75,1).
Is dened by x(0)
i(t)=u(0)
ri (t)+λ(0)
ri ,t[0.25(r1),0.25r),r=1:4,x
(0)
i(1) = lim
t10u(0)
4i(t)+λ(0)
4i,
i=1,2,the vector function x(0)(t)=x(0)
1(t),x
(0)
2(t). The inequality ||xx(0)||0<0.001 is true.
Solve the system of equations Q3(0.25)λ=F3(0.25) G3(u(0),0.25) on the 1st step.
Here G3(u(0),0.25) = (0,0.000145,0.000013,0.000004,0.000096,0.000066,0.000270,
0.000290).Find λ(1) =λ(1)
11
(1)
12
(1)
21
(1)
22
(1)
31
(1)
32
(1)
41
(1)
42 =(0.000000,1.000001,
0.187501,0.500011,0.250000,0.000000,0.187501,0.499999) and compute the components of
function system u(1)[t]:
u(1)
11 (t)=t2t+O(t),u
(1)
12 (t)=2t+O(t2),t[0,0.25),
u(1)
21 (t)=t2t+0.1875027 + O(t),u
(1)
22 (t)=2t0.4999997 + O(t2),t[0.25,0.5),
u(1)
31 (t)=t2t+0.25 + O(t),u
(1)
32 (t)=2t1+O(t2),t[0.5,0.75),
u(1)
41 (t)=t2t+0.1875071 + O(t),u
(1)
42 (t)=2t1.4999979 + O(t2),t[0.75,1).
Determine the vector function x(1) (t)=x(1)
1(t),x
(1)
2(t)by the equalities:
x(1)
i(t)=u(1)
ri (t)+λ(1)
ri ,t[0.25(r1),0.25r),r=1:4,i=1,2,
x(1)
i(1) = lim
t10u(1)
4i(t)+λ(1)
4i,i=1,2,
and obtain the estimate ||xx(1) ||00.0000122 <0.0001.
Thus, for the problem (14), (15) considered on [0,1],theoered algorithm with ν=3,h=0.25 gives
on rst step the approximate solution up to ε=0.0001.
Calculations are made in the mathematical package MathCAD 15.
FUNDING
This research has was funded by the Science Committee of the Ministry of Education and Science of
the Republic of Kazakhstan (grant no. AP08956612).
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LOBACHEVSKII JOURNAL OF MATHEMATICS Vol. 42 No. 3 2021
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In this paper, a new computational approach is presented to solve a boundary-value problem for a differential equation with piecewise constant argument of generalized type (DEPCAG). The presented technique is based on the Dzhumabaev parametrization method. A useful numerical algorithm is developed to obtain the numerical values from the problem. Numerical experiments are conducted to demonstrate the accuracy and efficiency.
... Бұл мақалада импульсті жүктелген дифференциалдық теңдеулер жүйесі үшін параметрлі шеттік есепті шешу үшін профессор Жұмабаев ұсынған параметрлеу әдісінің [18,19] сандық жүзеге асырылуы қолданылады. Осы параметрлеу әдісін дифференциалдық теңдеулердің әртүрлі кластары үшін есептерді шешуде қолдануын [20][21][22][23][24][25] Ұсынылып отырған сандық әдіс (11) жүйені құруға және шешуге негізделген. (9), (10) теңдеулерінен көрініп тұрғандай (11) жүйенің коэффициенттері мен оң жағы жәй дифференциалдық теңдеулер үшін матрицалық және векторлық Коши есептерінің шешімі ретінде: (13) . ...
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The boundary value problem depending on the parameter for the system of impulsive loaded differential equations is considered. Algorithms of numerical realization of the Dzhumabaev parameterization method are developed for numerical solving of the studied boundary value problem depending on the parameter. Algorithms of numerical realization of the Dzhumabaev parameterization method are based on the solving of Cauchy problems for the system of ordinary differential equations. As a result of application of the proposed method, finding a solution to the boundary value problem depending on the parameter for impulsive loaded differential equations leads to finding a solution to the system of algebraic equations. This system of algebraic equations consists of a boundary condition and equalities with respect to the conditions at the impulsive points. Numerical results showing the high efficiency of the numerical implementation of the Dzhumabaev parameterization method are given. The result demonstrate that there is congruence between the numerical and the exact results to a high order of accuracy.
... This article's basic objective is to broaden the modification of Dzhumabaev parametrization method [7], [8] to the boundary value problem for the system of loaded DEPCAG. For this purpose, we have developed computational method solving a boundaryvalue problem for the system of loaded DEPCAG. ...
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In this paper, modification of Dzhumabaev parameterization method is developed to a boundary value problem for systems of loaded differential equations with piecewise constant argument of generalized type (EPCAG). The method is based on reducing the considering problem to an equivalent multi-point boundary value problem for ordinary differential equations with parameters. An equivalent boundary value problem with parameters consists of the Cauchy problem for a system of ordinary differential equations with parameters, a two-point condition, a continuity condition, and additional conditions for a piecewise constant argument. The solution of the Cauchy problem for a system of ordinary differential equations with parameters is constructed using the fundamental matrix of the differential equation. A system of linear algebraic equations for the parameters is compiled using the values of the solution at the corresponding points and substituting them into the two-point condition, the continuity condition, and the conditions for the piecewise constant argument. A modification of Dzhumabaev parameterization method for solving the considering boundary value problem is proposed which is based on solving the constructed system and the 4th order Runge-Kutta method for solving the Cauchy problem on subintervals. The obtained results are verified by a numerical example. Numerical analysis showed high efficiency of the constructed modification of Dzhumabaev parameterization method.
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In this paper, a new technique, namely the Dzhumabaev parameterization method, is presented and applied to linear boundary value problem with parameter for delay differential equation to find an efficient algorithm for their approximate solutions. Effectiveness of this algorithm is tested by examples of second-order delay differential equations and linear boundary value problem with parameter for delay differential equations. Obtained results reveal that proposed algorithm of the Dzhumabaev parameterization method is highly efficient and straightforward to execute.
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This paper considers a family of linear two-point boundary value problems for systems of ordinary differential equations. The questions of existence of its solutions are investigated and methods of finding approximate solutions are proposed. Sufficient conditions for the existence of a family of linear two-point boundary value problems for systems of ordinary differential equations are established. The uniqueness of the solution of the problem under consideration is proved. Algorithms for finding an approximate solution based on modified of the algorithms of the D.S. Dzhumabaev parameterization method are proposed and their convergence is proved. According to the scheme of the parameterization method, the problem is transformed into an equivalent family of multipoint boundary value problems for systems of differential equations. By introducing new unknown functions we reduce the problem under study to an equivalent problem, a Volterra integral equation of the second kind. Sufficient conditions of feasibility and convergence of the proposed algorithm are established, which also ensure the existence of a unique solution of the family of boundary value problems with parameters. Necessary and sufficient conditions for the well-posedness of the family of linear boundary value problems for the system of ordinary differential equations are obtained.
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This textbook provides a rigorous and lucid introduction to the theory of ordinary differential equations (ODEs), which serve as mathematical models for many exciting real-world problems in science, engineering, and other disciplines. Key Features of this textbook: Effectively organizes the subject into easily manageable sections in the form of 42 class-tested lectures Provides a theoretical treatment by organizing the material around theorems and proofs Uses detailed examples to drive the presentation Includes numerous exercise sets that encourage pursuing extensions of the material, each with an "answers or hints" section Covers an array of advanced topics which allow for flexibility in developing the subject beyond the basics Provides excellent grounding and inspiration for future research contributions to the field of ODEs and related areas This book is ideal for a senior undergraduate or a graduate-level course on ordinary differential equations. Prerequisites include a course in calculus. Series: Universitext Ravi P. Agarwal received his Ph.D. in mathematics from the Indian Institute of Technology, Madras, India. He is a professor of mathematics at the Florida Institute of Technology. His research interests include numerical analysis, inequalities, fixed point theorems, and differential and difference equations. He is the author/co-author of over 800 journal articles and more than 20 books, and actively contributes to over 40 journals and book series in various capacities. Donal O’Regan received his Ph.D. in mathematics from Oregon State University, Oregon, U.S.A. He is a professor of mathematics at the National University of Ireland, Galway. He is the author/co-author of 14 books and has published over 650 papers on fixed point theory, operator, integral, differential and difference equations. He serves on the editorial board of many mathematical journals. Previously, the authors have co-authored/co-edited the following books with Springer: Infinite Interval Problems for Differential, Difference and Integral Equations; Singular Differential and Integral Equations with Applications; Nonlinear Analysis and Applications: To V. Lakshmikanthan on his 80th Birthday. In addition, they have collaborated with others on the following titles: Positive Solutions of Differential, Difference and Integral Equations; Oscillation Theory for Difference and Functional Differential Equations; Oscillation Theory for Second Order Linear, Half-Linear, Superlinear and Sublinear Dynamic Equations.
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Preface. 1: Continuous Problems. 1.1. Introduction. 1.2. Abel-Gontscharoff Interpolation. 1.3. Solution of Linear Problems. 1.4. Existence and Uniqueness. 1.5. Picard's and Approximate Picard's Methods. 1.6. Quasilinearization and Approximate Quasilinearization. 1.7. Integro-Differential Equations. 1.8. Delay-Differential Equations. 1.9. Necessary and Sufficient Conditions for Right Disfocality. 1.10. Tests for Right and Eventual Disfocalities. 1.11. Green's Functions. 1.12. Monotone Convergence. 1.13. Uniqueness Implies Uniqueness. 1.14. Uniqueness Implies Existence. 1.15. Continuous Dependence and Differentiation with respect to Boundary Values. 1.16. Right Disfocality Implies Right Disfocality. 1.17. Right Disfocality Implies Existence. 1.18. Differential Inequalities Imply Existence. 1.19. Infinite Interval Problems. 1.20. Best Possible Results: Control Theory Methods. 1.21. Converse Theorems. 1.22. Focal Subfunctions. 1.23. Generalized Problem I. 1.24. Generalized Problem II. 1.25. A Singular Problem. 1.26. A Problem with Impulse Effects. Comments and Remarks. References. 2: Discrete Problems. 2.1. Introduction. 2.2. Discrete Abel-Gontscharoff Interpolation. 2.3. Existence and Uniqueness. 2.4. Picard's and Approximate Picard's Methods. 2.5. Quasilinearization and Approximate Linearization. 2.6. Necessary and Sufficient Conditions for Right Disfocality. 2.7. Tests for Right and Eventual Disfocalities. 2.8. Green's Functions. 2.9. Monotone Convergence. 2.10. Continuous Dependence and Differentiation with Respect to Initial and Boundary Values. 2.11. Differences with Respect to Boundary Points. 2.12. Uniqueness Implies Existence. 2.13. Generalized Problems. Comments and Remarks. References. Index.
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