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 
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 Which completes the proof. 
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