1.3 Existence Methods
1.3.1 The Contraction Mapping Theorem
Here we prove a very useful fixed point theorem called the
contraction mapping theorem. We will apply this theorem to prove the existence
and uniqueness of solutions of our nonlinear problem.
Definition 1.3.1 Let f : X - X be a map of a metric space to
itself. A point x 2 X is called a fixed point off if f(x) = x.
Definition 1.3.2 Let (X, dx) and (Y, dY ) be metric spaces. A map
çü : X -p Y is called a contraction if there exists a positive
number C < 1 such that
dy (ço(x),ço(y)) Cdx(x,y), (1.35)
for all x,y 2 X.
Theorem 1.3.1 (Contraction mapping theorem [45] )
Let (X, d) be a complete metric space. If çü : X -p X
is a contraction, then çü has a unique fixed point.
1.3.2 Gronwell's lemma
Theorem 1.3.2 ( In integral form)
Let T > 0, and let çü be a function such that,
çü 2 L1(0, T), çü ~ 0, almost everywhere and
q be a function such that, q 2 L1(0,T), q ~ 0, almost everywhere and
qço 2 L1 [0, T], Ci, C2 ~ 0. Suppose that
q(t) ~ Ci + C2 Zt ço(s)q(s)ds, for a.e t 2
]0,T[, (1.36)
0
then,
t
0 1
f
0
q(t) Ci exp @C2 '(s)ds A , for a.e t 2
]0,T[. (1.37)
Proof. Let
F(t) = C1 + C2 Zt ço(s)q(s)ds, for t 2 [0, T],
(1.38)
0
we have,
q(t) F(t),
From (1.38) we have
F'(t) = C2ço(t)q(t)
~ C2ço(t)A(t), for a.e t 2 ]0,T[. (1.39)
d
8
<
:
dt
Consequently,
0 1 9
f t =
F (t) exp @_ C2'(s)ds A 0, (1.40)
0
;
then,
t
0 1
f
F (t) ~ Ci exp @C2 (s)ds A , for a.e t 2
]0, T[. (1.41)
0
Since q F, then our result holds.
In particle, if C1 = 0, we have q = 0 for almost everywhere t 2
]0, T[.
1.3.3 The mean value theorem
Theorem 1.3.3 Let G : [a, b] -p be a continues function and
çü : [a, b] -p is an integral positive function, then there exists
a number x in (a, b) such that
Zb G(t)cp(t)dt = G(x) Zb ço(t)dt.
(1.42)
a a
m Zb ço(t)dt ~ Zb G(t)ço(t)dt
M Zb ço(t)dt. (1.46)
a a a
In particular for ço(t) = 1, there exists x 2 (a, b) such
that
Zb G(t)dt = G(x) (b - a). (1.43)
a
Proof. Let
m = inf {G(x), x 2 [a, b]} (1.44)
and
M = sup {G(x), x 2 [a, b]} (1.45)
of course m and M exist since [a, b] is compact. Then, it follows
that
By monotonicity of the integral. dividing through by f a b
ço(t)dt, we have that
f a b G(t)cp(t)dt
m < f b < M. (1.47)
a co(t)dt
Since G(t) is continues, the intermediate value theorem implies
that there exists x 2 [a, b] such that
: (1.48)
a co(t)dt
f a b C(t)'(t)dt G(x) = f b
Which completes the proof.
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