On Application of the Fixed-Point Theorem to the Solution of Ordinary Differe...BRNSS Publication Hub
We know that a large number of problems in differential equations can be reduced to finding the solution x to an equation of the form Tx=y. The operator T maps a subset of a Banach space X into another Banach space Y and y is a known element of Y. If y=0 and Tx=Ux−x, for another operator U, the equation Tx=y is equivalent to the equation Ux=x. Naturally, to solve Ux=x, we must assume that the range R (U) and the domain D (U) have points in common. Points x for which Ux=x are called fixed points of the operator U. In this work, we state the main fixed-point theorems that are most widely used in the field of differential equations. These are the Banach contraction principle, the Schauder–Tychonoff theorem, and the Leray–Schauder theorem. We will only prove the first theorem and then proceed.
On Application of the Fixed-Point Theorem to the Solution of Ordinary Differe...BRNSS Publication Hub
We know that a large number of problems in differential equations can be reduced to finding the solution x to an equation of the form Tx=y. The operator T maps a subset of a Banach space X into another Banach space Y and y is a known element of Y. If y=0 and Tx=Ux−x, for another operator U, the equation Tx=y is equivalent to the equation Ux=x. Naturally, to solve Ux=x, we must assume that the range R (U) and the domain D (U) have points in common. Points x for which Ux=x are called fixed points of the operator U. In this work, we state the main fixed-point theorems that are most widely used in the field of differential equations. These are the Banach contraction principle, the Schauder–Tychonoff theorem, and the Leray–Schauder theorem. We will only prove the first theorem and then proceed.
Mathematics (from Greek μάθημα máthēma, “knowledge, study, learning”) is the study of topics such as quantity (numbers), structure, space, and change. There is a range of views among mathematicians and philosophers as to the exact scope and definition of mathematics
Antibacterial Application of Novel Mixed-Ligand Dithiocarbamate Complexes of ...IOSR Journals
Nine stable mixed ligand dithiocarbamate complexes of Nickel (II) ion were prepared. The complexes were characterized with electronic spectroscopy, infrared spectroscopy, conductance measurement, melting point and percentage metal analysis. Resulting analytical data gave credence to the assignment of a tentative square planar geometry to all the complexes. The complexes were proposed to have a general formulae of [Ni(Sal)(Rdtc)], where Sal = salicylaldehyde; R = dibenzylamine(Bz2NH), methylphenylamine(MePhNH),pyrrolidineamine(pyrrolNH),piperidineamine(piperNH),morpholineamine(MorpNH), anilineamine(AnilNH), para-chloroanilineamine(p-ClAnilNH), toludineamine(TolNH) and anisidineamine(AnisNH); and dtc = dithiocarbamate anion. The metal complexes were screened against six different bacteria strain using Agar diffusion method. The antibacterial studies reveal that the metal complexes exhibit broad spectrum antibacterial activity against Escherichia coli, Staphylococcus aureus, Klebsiella oxytoca and Pseudomonas aureginosa with inhibitory range of 10.5.—20.0mm.
Mathematics (from Greek μάθημα máthēma, “knowledge, study, learning”) is the study of topics such as quantity (numbers), structure, space, and change. There is a range of views among mathematicians and philosophers as to the exact scope and definition of mathematics
Antibacterial Application of Novel Mixed-Ligand Dithiocarbamate Complexes of ...IOSR Journals
Nine stable mixed ligand dithiocarbamate complexes of Nickel (II) ion were prepared. The complexes were characterized with electronic spectroscopy, infrared spectroscopy, conductance measurement, melting point and percentage metal analysis. Resulting analytical data gave credence to the assignment of a tentative square planar geometry to all the complexes. The complexes were proposed to have a general formulae of [Ni(Sal)(Rdtc)], where Sal = salicylaldehyde; R = dibenzylamine(Bz2NH), methylphenylamine(MePhNH),pyrrolidineamine(pyrrolNH),piperidineamine(piperNH),morpholineamine(MorpNH), anilineamine(AnilNH), para-chloroanilineamine(p-ClAnilNH), toludineamine(TolNH) and anisidineamine(AnisNH); and dtc = dithiocarbamate anion. The metal complexes were screened against six different bacteria strain using Agar diffusion method. The antibacterial studies reveal that the metal complexes exhibit broad spectrum antibacterial activity against Escherichia coli, Staphylococcus aureus, Klebsiella oxytoca and Pseudomonas aureginosa with inhibitory range of 10.5.—20.0mm.
Recent Developments and Analysis of Electromagnetic Metamaterial with all of ...IOSR Journals
Recent advances in metamaterials (MMs) research have highlighted the possibility to create novel
devices with electromagnetic functionality. The metamaterial have the power which can easily construct
materials with a user-designed EM response with a particular target frequency. This is the important
phenomena of THz frequency region that can make a considerable progress in design fabrication, and define the
characteristics of MMs at THz frequencies. This article illustrates the latest advancements of THz MMs
research.
On Analytic Review of Hahn–Banach Extension Results with Some GeneralizationsBRNSS Publication Hub
The useful Hahn–Banach theorem in functional analysis has significantly been in use for many years ago. At this point in time, we discover that its domain and range of existence can be extended point wisely so as to secure a wider range of extendibility. In achieving this, we initially reviewed the existing traditional Hahn–Banach extension theorem, before we carefully and successfully used it to generate the finite extension form as in main results of section three.
On the Application of a Classical Fixed Point Method in the Optimization of a...BRNSS Publication Hub
This work on classical optimization reveals the Newton’s fixed point iterative method as involved in
the computation of extrema of convex functions. Such functions must be differentiable in the Banach
space such that their solution exists in the space on application of the Newton’s optimization algorithm
and convergence to the unique point is realized. These results analytically were carried as application
into the optimization of a multieffect evaporator which reveals the feasibility of theoretical and practical
optimization of the multieffect evaporator.
On Frechet Derivatives with Application to the Inverse Function Theorem of Or...BRNSS Publication Hub
In this paper, the Frechet differentiation of functions on Banach space was reviewed. We also investigated that it is algebraic properties and its relation by applying the concept to the inverse function theorem of the ordinary differential equations. To achieve the feat, some important results were considered which finally concluded that the Frechet derivative can extensively be useful in the study of ordinary differential equations.
Richard's aventures in two entangled wonderlandsRichard Gill
Since the loophole-free Bell experiments of 2020 and the Nobel prizes in physics of 2022, critics of Bell's work have retreated to the fortress of super-determinism. Now, super-determinism is a derogatory word - it just means "determinism". Palmer, Hance and Hossenfelder argue that quantum mechanics and determinism are not incompatible, using a sophisticated mathematical construction based on a subtle thinning of allowed states and measurements in quantum mechanics, such that what is left appears to make Bell's argument fail, without altering the empirical predictions of quantum mechanics. I think however that it is a smoke screen, and the slogan "lost in math" comes to my mind. I will discuss some other recent disproofs of Bell's theorem using the language of causality based on causal graphs. Causal thinking is also central to law and justice. I will mention surprising connections to my work on serial killer nurse cases, in particular the Dutch case of Lucia de Berk and the current UK case of Lucy Letby.
THE IMPORTANCE OF MARTIAN ATMOSPHERE SAMPLE RETURN.Sérgio Sacani
The return of a sample of near-surface atmosphere from Mars would facilitate answers to several first-order science questions surrounding the formation and evolution of the planet. One of the important aspects of terrestrial planet formation in general is the role that primary atmospheres played in influencing the chemistry and structure of the planets and their antecedents. Studies of the martian atmosphere can be used to investigate the role of a primary atmosphere in its history. Atmosphere samples would also inform our understanding of the near-surface chemistry of the planet, and ultimately the prospects for life. High-precision isotopic analyses of constituent gases are needed to address these questions, requiring that the analyses are made on returned samples rather than in situ.
Observation of Io’s Resurfacing via Plume Deposition Using Ground-based Adapt...Sérgio Sacani
Since volcanic activity was first discovered on Io from Voyager images in 1979, changes
on Io’s surface have been monitored from both spacecraft and ground-based telescopes.
Here, we present the highest spatial resolution images of Io ever obtained from a groundbased telescope. These images, acquired by the SHARK-VIS instrument on the Large
Binocular Telescope, show evidence of a major resurfacing event on Io’s trailing hemisphere. When compared to the most recent spacecraft images, the SHARK-VIS images
show that a plume deposit from a powerful eruption at Pillan Patera has covered part
of the long-lived Pele plume deposit. Although this type of resurfacing event may be common on Io, few have been detected due to the rarity of spacecraft visits and the previously low spatial resolution available from Earth-based telescopes. The SHARK-VIS instrument ushers in a new era of high resolution imaging of Io’s surface using adaptive
optics at visible wavelengths.
Richard's entangled aventures in wonderlandRichard Gill
Since the loophole-free Bell experiments of 2020 and the Nobel prizes in physics of 2022, critics of Bell's work have retreated to the fortress of super-determinism. Now, super-determinism is a derogatory word - it just means "determinism". Palmer, Hance and Hossenfelder argue that quantum mechanics and determinism are not incompatible, using a sophisticated mathematical construction based on a subtle thinning of allowed states and measurements in quantum mechanics, such that what is left appears to make Bell's argument fail, without altering the empirical predictions of quantum mechanics. I think however that it is a smoke screen, and the slogan "lost in math" comes to my mind. I will discuss some other recent disproofs of Bell's theorem using the language of causality based on causal graphs. Causal thinking is also central to law and justice. I will mention surprising connections to my work on serial killer nurse cases, in particular the Dutch case of Lucia de Berk and the current UK case of Lucy Letby.
What is greenhouse gasses and how many gasses are there to affect the Earth.moosaasad1975
What are greenhouse gasses how they affect the earth and its environment what is the future of the environment and earth how the weather and the climate effects.
Multi-source connectivity as the driver of solar wind variability in the heli...Sérgio Sacani
The ambient solar wind that flls the heliosphere originates from multiple
sources in the solar corona and is highly structured. It is often described
as high-speed, relatively homogeneous, plasma streams from coronal
holes and slow-speed, highly variable, streams whose source regions are
under debate. A key goal of ESA/NASA’s Solar Orbiter mission is to identify
solar wind sources and understand what drives the complexity seen in the
heliosphere. By combining magnetic feld modelling and spectroscopic
techniques with high-resolution observations and measurements, we show
that the solar wind variability detected in situ by Solar Orbiter in March
2022 is driven by spatio-temporal changes in the magnetic connectivity to
multiple sources in the solar atmosphere. The magnetic feld footpoints
connected to the spacecraft moved from the boundaries of a coronal hole
to one active region (12961) and then across to another region (12957). This
is refected in the in situ measurements, which show the transition from fast
to highly Alfvénic then to slow solar wind that is disrupted by the arrival of
a coronal mass ejection. Our results describe solar wind variability at 0.5 au
but are applicable to near-Earth observatories.
Earliest Galaxies in the JADES Origins Field: Luminosity Function and Cosmic ...Sérgio Sacani
We characterize the earliest galaxy population in the JADES Origins Field (JOF), the deepest
imaging field observed with JWST. We make use of the ancillary Hubble optical images (5 filters
spanning 0.4−0.9µm) and novel JWST images with 14 filters spanning 0.8−5µm, including 7 mediumband filters, and reaching total exposure times of up to 46 hours per filter. We combine all our data
at > 2.3µm to construct an ultradeep image, reaching as deep as ≈ 31.4 AB mag in the stack and
30.3-31.0 AB mag (5σ, r = 0.1” circular aperture) in individual filters. We measure photometric
redshifts and use robust selection criteria to identify a sample of eight galaxy candidates at redshifts
z = 11.5 − 15. These objects show compact half-light radii of R1/2 ∼ 50 − 200pc, stellar masses of
M⋆ ∼ 107−108M⊙, and star-formation rates of SFR ∼ 0.1−1 M⊙ yr−1
. Our search finds no candidates
at 15 < z < 20, placing upper limits at these redshifts. We develop a forward modeling approach to
infer the properties of the evolving luminosity function without binning in redshift or luminosity that
marginalizes over the photometric redshift uncertainty of our candidate galaxies and incorporates the
impact of non-detections. We find a z = 12 luminosity function in good agreement with prior results,
and that the luminosity function normalization and UV luminosity density decline by a factor of ∼ 2.5
from z = 12 to z = 14. We discuss the possible implications of our results in the context of theoretical
models for evolution of the dark matter halo mass function.
Earliest Galaxies in the JADES Origins Field: Luminosity Function and Cosmic ...
On Local Integrable Solutions of Abstract Volterra Integral Equations
1. IOSR Journal of Mathematics (IOSR-JM)
e-ISSN: 2278-5728, p-ISSN: 2319-765X. Volume 11, Issue 1 Ver. III (Jan - Feb. 2015), PP 25-32
www.iosrjournals.org
DOI: 10.9790/5728-11132532 www.iosrjournals.org 25 |Page
On Local Integrable Solutions of Abstract Volterra Integral
Equations
Atanaska Georgieva1
, Lozanka Trenkova2
1 2
(Faculty of Mathematics and Informatics, Plovdiv University, Bulgaria,
Abstract: The aim of this paper is to study the existence and uniqueness of solution of abstract Volterra
integral equations of the second kind in complete locally convex topological space. An example illustrating the
obtained result is given.
Keywords: Abstract Volterra integral equations, locally integrable solution
I. Introduction
Integral equations have a lot of applications in physics, engineering, mechanics, biology, and
economics (cf., e.g.[1–7,11] and references therein). By applying the theory of fixed point, some interesting
results on the existence of locally integrable solutions of abstract Volterra integral equations are obtained under
certain conditions, see, e.g. [2,3,7] and the references therein.
In this work we consider the abstract Volterra integral equations of first and second kind in the case
when the independent variable belongs to a topological space. We find sufficient conditions for existence and
uniqueness of the trivial solution of the homogeneous equation and sufficient conditions for existence and
uniqueness of local integrable solution of the non homogeneous equations. Moreover, we give an example,
which shows that the investigated equation has a unique locally integrable solution.
II. Preliminaries
Let be a topological space, 2B
denotes the - algebra of the Borel subsets of and let
: [0, )B
be a nontrivial -finite Borel measure.
We introduce the map : 2M
which associates every point x a closed subset x
M and let
denote the set { : }x
M x M .
We will say that the condition (A) hold if for the map : 2M
the following conditions are fulfilled:
A1. For every x
M M the following is fulfilled
sup ( ) .x
x
M
A2. For any x and x
y M the inclusion y x
M M holds.
A3. For every x and for every nonempty open subset x
O of x
M there exists a neighbourhood
, x
W W x O , such that for every y W the following holds
.y x
M O
A4. There exists a point 0
x such that 0
0x
M .
Let B be a real Banach space with norm||.||B .
Consider the linear space
1 1
( , )loc loc
L L B , where
1
( , ) { : , ( ) }
x
loc yB
M
L B f B f is strongly measurable and f y d for every x
We introduce topology
1
locF using a family of semi-norms
|| || ( )x
x
M yB
M
f f y d
for x and
1
loc
f L .
2. On local integrable solution of an abstract Volterra integral equations
DOI: 10.9790/5728-11132532 www.iosrjournals.org 26 |Page
Then by theorem 3.5.4[10] and theorem 1(Ch. VII, §1)[12] it follows that
1
loc
L is a complete locally convex
topological space.
Let A be an ordered index set and
1
{ } A locf L ,
1
0 locf L .
Proposition 1.[9] A sequence
1
{ } A locf L is convergent to
1
0 locf L in the topology
1
locF if and only if
0lim 0
xM
f f
for x .
Definition 2.1. We say that the function
1
loc
f L is M almost separable - valued if for every x and
x
M M there exists a set x x
E M , 0x
E , such that ( )x x
f M E is separable subset of B .
We will say that the operator 1 1
: loc loc
Q L L is continuous and satisfies the conditions (B) if the
following conditions are fulfilled:
B1. For every ,x y and
1
1 2
, loc
f f L we have
1 2 1 2
( , , ( ) ( )) ( , , ( )) ( , , ( ))Q x y f y f y Q x y f y Q x y f y
B1*. For every ,x y and
1
1 2
, loc
f f L there exists a constant 0x
L , such that
1 2 1 2
( , , ( )) ( , , ( )) ( ) ( )
x x
y x yB B
M M
Q x y f y Q x y f y d L f y f y d
B2. For every x there exists a constant 0x
A , such that for every
1
loc
f L and y the inequality
( , , ( )) ( )
x x
y x yB B
M M
Q x y f y d A f y d holds.
B3. For every 0 , x and
1
loc
f L there exists a neighbourhood , ,W W x f of the point x ,
such that for every y W the inequality
( , , ( )) ( , , ( )) ( )
x y x y
z zB B
M M M M
Q x z f z Q y z f z d f z d
holds.
B4. For every 0 , x and
1
loc
f L there exists a neighbourhood , ,V V x f of the point x ,
such that for every y V the inequality
( )
x y
zB
M M
f z d
holds, where { } { }x y x y y xM M M M M M .
B5. For every fixed element x and every fixed function
1
loc
f L the mapping
( ) , , ( )f
y Q x y f y is M almost separable – valued and weakly measurable with respect to x
M for
x .
Remark 1: If for the operator Q condition (B1*) hold and ( , ,0) 0Q x y for every ,x y , then
condition (B2) is a consequence of condition (B1*).
III. Main Results
We consider the equations
( ) ( )( )f x Kf x (3.1)
and
( ) ( ) ( )( )f x x Kf x (3.2)
where
1
, loc
f L , and operator
1 1
: loc loc
K L L is defined by the equality
3. On local integrable solution of an abstract Volterra integral equations
DOI: 10.9790/5728-11132532 www.iosrjournals.org 27 |Page
( )( ) ( , , ( )) ,
x
y
M
Kf x Q x y f y d (3.3)
where x
M M .
Since for every linear and continuous functional
*
defined on B the map
*
, :f is measurable
on every x
M M , then the existence of the integral in (3.3) is guaranteed by the conditions (B) and the
theorems 3.4.7, p.94 and 3.5.3, p.86 in [10]
Theorem 3.1. Let the conditions (A1), (B2), (B3), (B4) and (B5) hold. Then for any
1
loc
f L the function
( )Kf x is continuous in .
Proof: Let 1
,x x and
1
loc
f L . The constants x
A and 1x
A are defined in condition (B2).
Let 1
1
1
max{sup ,sup }
x x
x x
x M x M
A A A
.
Let 0 be an arbitrary number. Condition (B3) implies that there exists a neighbourhood
1
1
, ,
xM
W x f
f
of the point 1
x , such that for every
1
1
, ,
xM
x W x f
f
the following inequality
1 1
1
( , , ( )) ( , , ( ))
2x x x
zB
M M M
Q x z f z Q x z f z d
f
(3.4)
holds.
Condition (B4) implies that there exists a neighbourhood 1
, ,V x f of the point 1
x , such that for every
1
, ,x V x f the following estimate
1 1
( )
2x x
zB
M M
f z d
A
(3.5)
holds.
Let 1 1 1
, , , , , ,U x f W x f V x f and 1
, ,x U x f . Then the inequalities (3.4),
(3.5) and condition (B2) yield that
1 1
1
1
1
1
1 1
1
111
|| ( ) ( ) || ( , , ( )) ( , , ( ))
|| ( , , ( )) ( , , ( )) ||
|| ( , , ( )) || || ( , , ( )) ||
|| ( ) || || ( ) ||
2
B
M Mx x B
B y
Mx M x
B y B y
M M M Mx x x x
B y x B y x
M MM M x xM x xx
Kf x Kf x Q x y f y Q x y f y
Q x y f y Q x y f y d
Q x y f y d Q x y f y d
f y d A f y d A
f
1
1
1
11
|| ( ) ||
|| ( ) ||
2
B y
M Mx x
B yM Mx x
M MM x xx
f y d
f A f y d
f
holds.
4. On local integrable solution of an abstract Volterra integral equations
DOI: 10.9790/5728-11132532 www.iosrjournals.org 28 |Page
Theorem 3.2. Let the following conditions are fulfilled:
1. The conditions (A1), (B1), (B2) and (B5) hold.
2. There exists a constant 2
sup
z
x
x M
A A
for each z.
Then the operator K maps
1
loc
L into
1
loc
L continuously.
Proof: Let
1
loc
f L . First we will prove that
1
loc
Kf L .
Let z. Condition (A1) and (B2) imply that
2
|| || ( ) || ( , , ( )) ||
( , , ( ))
M x y B xBz
M M Mz z x
y x x xB M x
M M Mz x z
xM x
M z
Kf Kf x d Q x y f y d d
Q x y f y d d A f d
A f d
holds.
Therefore we get that
1
loc
Kf L .
Now, we will prove that K is continuous.
Let A be an ordered index set, 0lim f f
,
1
{ } A locf L ,
1
0 locf L and let z. Then we have
0 0
0
0 0
0
|| || ( ) ( )
|| ( , , ( )) ( , , ( )) ||
( , , ( ) ( )) ( ) ( )
M xBz
M z
y B x
M Mz x
y x x y xB B
M M M Mz x z x
x xM x
M z
Kf Kf Kf x Kf x d
Q x y f y Q x y f y d d
Q x y f y f y d d A f y f y d d
A f f d
holds. Therefore we get that 0
|| || 0Mz n
Kf Kf
.
Theorem 3.3. Let the following conditions are fulfilled:
1. The conditions (A) and (B) hold.
2. The condition 2 of Theorem 3.2 holds.
3. The space is connected.
Then the equation (3.1) has only the trivial solution 0f for .
Proof: Let
*
f be an arbitrary solution of (3.1), be an arbitrary real number and let consider the set
*
*
{ : ( ) 0 }xf
N x f y for y M .
Condition (A4) implies that there exist an element 0x , such that 0
( ) 0xM .
Let 0
( )xM (the case 0
( )xM is trivial). Condition (A2) yields that for every 0xx M we have
0
( ) 0xM i.e. *0 f
x N and therefore *
f
N .
Now we will prove that *
f
N is a closed set.
Let *{ }n f
x N be an arbitrary convergent sequence and let
*
x be its limit in .
If *
x
M then we have *
*
f
x N . Let *
x
M , *
x
z M be an arbitrary fixed point and 0 be an
arbitrary number.
5. On local integrable solution of an abstract Volterra integral equations
DOI: 10.9790/5728-11132532 www.iosrjournals.org 29 |Page
From Theorem 3.1 it follows that
*
f is continuous function in and therefore there exists a neighbourhood
*
, ,W W z f of the point z , such that for every y W we have
* *
( ) ( ) B
f y f z .
The condition (A3) implies that for the set x x
O W M there exists a neighbourhood *
U x of the point
*
x , such that for every
*
( )y U x we have *y x
M O
There exists a number 0n , such that for 0n n , *
n
x U x and *
nx x
M O .
Let *
*
nx x
y M O
for any 0n n . Taking into account that
* *
( ) 0f y , then we have
*
( ) B
f z
i.e.
*
( ) 0f z . Therefore *
*
f
x N and we conclude that *
f
N is closed set.
Now, we will prove that *
f
N is open set. Let *
f
a N be an arbitrary.
Condition (B4) yields that there exists a neighbourhood ,V V a , such that for every x V and every
1
locf L the following estimate
( ) yB
M Mx a
f y d
holds.
Let b V . Denote by
1
( )loc bL M the Banach space of functions , which are strongly measurable and integrable
in bM with norm
( ) yM Bb
Mb
g g y d
We consider the set
1
{ ( ) : ( ) 0 }loc b a b
T g L M g x for x M M .
Obviously, T is a closed subset of
1
( )loc bL M and the restriction of
*
f over bM is contained in it. For every
a b
x M M and g T conditions (A2) implies that
( )( ) ( , , ( )) 0
x
y
M
Kg x Q x y g y d
i.e. K maps T into T .
Let 3
sup
b
x
x M
A A
. Let 1 2
,g g T be any elements and let 0
(0, ) , such that
0 3
1 2
1
2
bM
A
g g
. Then
we have
1 2 1 2
1 2
1 2
1 2
1 2
|| || ( ) ( )
|| ( , , ( )) ( , , ( )) ||
|| ( , , ( ) ( )) ||
|| ( , , ( ) ( )) ||
|| ( , , ( ) ( ) ||
M xBb
Mb
y B x
M Mb x
y B x
M M Mb x a
y B x
M M Mb x a
B y
M Mx a
Kg Kg Kg x Kg x d
Q x y g y Q x y g y d d
Q x y g y g y d d
Q x y g y g y d d
Q x y g y g y d d
1 2
1 2
0 3 0 1 2
|| ( ) ( ) ||
|| ( ) ( ) ||
1
2
x
Mb
x B y x
M M Mb x a
x B y x
M M Mb x a
x x Mb
Mb
A g y g y d d
A g y g y d d
A d A g g
6. On local integrable solution of an abstract Volterra integral equations
DOI: 10.9790/5728-11132532 www.iosrjournals.org 30 |Page
i.e. K is compressive over T and by Banach’s theorem it has only one fixed point 0
g T . Obviously,
0
( ) 0g x for bx M . Therefore *
f
b N i.e. *
f
N is open set.
Since is connected, then we get that *
f
N i.e.
*
( ) 0f x for every x .
This completes the proof of the Theorem.
Theorem 3.4 Let the following conditions are fulfilled:
1. The conditions of Theorem 3.3 hold.
2. The operator K is compact.
Then the equation (3.2) has exactly one solution for every
1
locL and for each .
Proof. The conditions of Theorem 3.4 immediately follow from Theorem 3.3, separability of
1
locL and
preposition 4, page 217 [14].
Suppose that
1
1 2
, loc
f f L are two different solutions of equation (3.2). Then for each x it follows
1 2 1 2
( ) ( )f x f x Kf x Kf x .
From conditions (B1) and (B2) it follows that for each x the inequality
1 2 1 2
1 2 1 2
( ) ( ) ( , , ( )) ( , , ( ))
( , , ( ) ( )) ( ) ( )
x
x x
yB B
M
y x yB B
M M
f x f x Q x y f y Q x y f y d
Q x y f y f y d A f y f y d
holds.
Using Theorem 2 and Theorem 3 from [5] we get 1 2
( ) ( ) 0B
f x f x for each x , which contradicts to
our supposition.
Remark: In the Theorem 3.2, Theorem 3.3 and Theorem 3.4 instead of condition (B1) we can use condition
(B1*).
We give an example, which illustrates the main result in the work i.e. Theorem 3.4.
Example: Let
2
[0, ) [0, ) , B , be Lebesgue measure. We define map : 2M
which associates every point 1 2
( , )x x x a set 1 2
[0, ] [0, ]x
M x x and the space
1
( , ) { : , ( ) }
x
loc yB
M
L B f B f is strongly measurable and f y d for every x .
Condition (A) is fulfilled for the map : 2M
.
Let the function :K is continuous. The operator
1 1
: loc locQ L L is defined by the
following equality
2
2
( )
( , , ( )) ( , )
1 ( )
f y
Q x y f y k x y
f y
We will show that for the operator Q the conditions (B) hold.
Let
1
1 2
, loc
f f L . Then the condition (B1*) is verified by
1 2
2 2
1 2
2 2
1 2
( , , ( )) ( , , ( ))
( ) ( )
( , )
1 ( ) 1 ( )
y
Mx
y
Mx
Q x y f y Q x y f y d
f y f y
k x y d
f y f y
7. On local integrable solution of an abstract Volterra integral equations
DOI: 10.9790/5728-11132532 www.iosrjournals.org 31 |Page
1 2 1 2
2 2
1 2
1 2
( ( ) ( ))( ( ) ( ))
( , )
(1 ( ))(1 ( ))
2 sup ( , ) ( ) ( )
y
M x
y
y M x M x
f y f y f y f y
k x y d
f y f y
k x y f y f y d
Condition (B2) is fulfilled because ( , ,0) 0Q x y for every ,x y .
Condition (B3) immediately follows from the continuity of function ( , )k x y .
Let 0, x and
1
locf L . From definition of the set ( )xM x it follows that there exists a
neighbourhood , ,V V x f of the point x , such that for y V the following
( )
x y
z
M M
f z d
is fulfilled. Consequently, the condition (B5) automatically holds.
Let the operator
1 1
: loc locK L L is defined by
2
2
( )
( )( ) ( , )
1 ( )x
y
M
f y
Kf x k x y d
f y
.
We will show that the operator K is compact.
We introduce topology
1
locF using a family of seminorms
1 2
1 2
1 2 2 1,
0 0
( , )
x x
x x
f f y y dy dy , for
1
locf L and 1 2, 0x x (*)
Let 1 0T , 2 0T . We denote the set 1 2[0, ] [0, ]D T T , the Banach space
1
{ : : ( ) }y
D
L D f D f is strongly measurable and f y d with norm
1
( ) y
D
f f y d and the operator of restriction 1 1
:D locL L D by ( ): |D Df f , i.e. ( )D f is
the restriction of the function
1
locf L to domain D .
Proposition 2.[9] A set
1
locC L is relatively compact in the topology
1
locF if and only if D C is relatively
compact in the Banach space 1
L D for 1 0T , 2 0T .
Let
1
1
{ ( ) : ( ) ( ) , , 1}DC g L D g x Kf x x D f
From Chapter VII, § 2, [13] follows that it is sufficient to show that the set C is uniformly bounded and
equicontinuous.
Let
1
1
( ), 1f L D f . Then
2
2 1( , ) ( , )
( , )
( )
( )( ) ( , ) max ( , ) ( ) max ( , )
1 ( )
max ( , ) .
y y
x y D D x y D D
D D
x y D D
f y
Kf x k x y d k x y f y d k x y f
f y
k x y for x D
Consequently, the set C is uniformly bounded.
Let ,x x D . Then
2
2
1
( )
( )( ) ( )( ) ( , ) ( , ) max ( , ) ( , ) ( )
1 ( )
max ( , ) ( , ) max ( , ) ( , )
y y
y D
D D
y D y D
f y
Kf x Kf x k x y k x y d k x y k x y f y d
f y
k x y k x y f k x y k x y
The function ( , )k x y is equicontinuous and therefore the set C is equicontinuous.
8. On local integrable solution of an abstract Volterra integral equations
DOI: 10.9790/5728-11132532 www.iosrjournals.org 32 |Page
References
[1]. Abdou M.A., Badr A.A., El-Kojok M.M., On the solution of a mixed nonlinear integral equation, Appl. Math. Comput. 217 (2011)
5466–5475.
[2]. Agarwal R.P., Banas J., Dhage B.C., Sarkate S.D., Attractivity results for a nonlinear functional integral equation, Georgian Math.
J. 18 (2011) 1–19.
[3]. Agarwal R.P., O’Regan D., Infinite Interval Problems for Differential, Difference and Integral Equations, Kluwer Academic
Publishers, Dordrecht, 2001.
[4]. Arfken G., H. Weber, Mathematical Methods for Physicists, Harcourt/Academic Press, 2000.
[5]. Bainov D.D., Myskis A.D., Zahariev A.I, On an abstract analog of the Belmann-Gronwall inequality, Publication of the Research
Institute for Mathematical science, Kyoto University, vol. 20, no. 5, 1984
[6]. Bainov D.D., Zahariev A.I, Kostadinov S.I., On an application of Fredholm`s alternative for nonlinear abstract integral equations,
Publication of the Research Institute for Mathematical science, Kyoto University, vol. 20, no. 5, 1984
[7]. Banas J. , Chlebowicz A., On integrable solutions of a nonlinear Volterra integral equation under Carathéodory conditions, Bull.
Lond. Math. Soc. 41 (6)(2009) 1073–1084.
[8]. Dieudonné J., Sur les espaces de Köthe, J. Anal. Math. 1 (1951) 81–115.
[9]. Engelking, R., General Topology. Heldermann, Berlin (1989)
[10]. Hille E., Phillips R.: Functional analysis and semi-groups. AMS, Colloquium Providence, 1957
[11]. Jung-Chan Chang, Cheng-Lien Lang, Chun-Liang Shih, Chien-Ning Yeh, Local existence of some nonlinear Volterra
integrodifferential equations with infinite delay, Taiwanese J. Math. 14 (2010) 131–152.
[12]. Kolmogorov A.N., Fomin S.,V., Elements of the Theory of Functions and Functional Analysis, Dover Publications,INC, Mineola,
New York, 1999
[13]. Maurin K., Methods of Hilbert spaces, Polish Scientific Publisher, Warsaw, 1972.
[14]. Robertson A., Robertson W., Topological Vector Spaces, Cambridge University Press, 1964
[15]. Zabrejko, P.P., Koshelev, A.I., Krasnosel’skii, M.A., Mikhlin, S.G.,Rakovshchik, L.S., Stecenko, V.J.: Integral Equations.
Noordhoff, Leyden(1975)