501 phys ِ prof. awatif ahmad hindi ُ enter reference 1- w.e boyce and r.c diprema,...
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501 PHYS
Prof. Awatif Ahmad Hindi
�Enter
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ReferenceReference1- W.E boyce and R.C Diprema , "elementary differential equations " 3rd edition (1975), johnwily2- E.A coddington , “ an introduction to ordinary differential equation “ , prentice –hali (1961) 3- E.Kreyszig “advanced engineering mathematics “ 7th edition , johnwily (1993)4- L.S. ross , “introduction to ordinary differential equations” 4th edition , john wily (1989)5- Abramowitz , M. stegun , I.A. hand book of mathematical function . dover, new York (1962)
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ReferenceReference
6- hochstadt , H. “special function of mathematical physics “ hold , rineheart , winstone , new york (1961)7- Lebedev,N.N.Special Functions and their Applications,Prentice-Hall,Englewood Cliffs,N.J.(1965)8-Rainvile,E.D.”Special Functions,Macmillan,New York(1960).
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Special Functions of mathematics
Integral Equation
Differential equation
contentscontents
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Definition
Properties of the Beta and Gamma functions:
some examples
Special Functions of mathematics Gamma and Beta functions
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DefinitionDefinition
We define the Gamma and Beta functions respectively by
0
11 1
0
( ) 0 (1)
( , ) (1 ) , , 0 (2)
t x t
x y
x e t dt x
B x y t t dt x y
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Properties of the Beta and Gamma Properties of the Beta and Gamma functions:functions:
2 2 1
0
(1) 1 (1)
( 1) ( ) 0 (2)
( 1) ! (3)
int
( ) 2 (4)t x
x x x x
x x
x is a nonnegative eger
x e t dt
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2
2 1 2 1
0
12
( ) ( )os sin (5)
2 ( )
( ) (6)
( ) ( )( , ) (7)
( )
( , ) ( , ) (8)
( 1, ) ( , ) ( )(9)
x y x yc d
x y
x
x yB x y
x y
B x y B y x
xB x y B x y i
x y
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( , 1) ( , ) ( )(9)yy xB x y B x y ii
2 12 12
sin( )
(2 ) ( ) ( ) (10)
( ) (1 ) (11)
x
x
x
x x x
x x
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Definition of the Gamma function for negative
values of the argument
Definition of the Gamma function for negative
values of the argument
12( ) ( 1)x x
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
12( ) ( 1)x x
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Some examplesSome examples
Express each of the following integrals in terms of Gamma or Beta functions and
simplify where possible
2
0
( ) tani d
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32
12
1
3 30
0
1
1
)1
) (1 )
1) ( )
1
t
dxii
x
iii t e dt
xiv dx
x
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Bessel FunctionsBessel Functions
Bessel’s equation of order n is
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
We shall solve (1)by using Frobinous method the solution of (1) is given by :
2
0
2
0
1( ) ( 1) ( ) (2)
! ( 1) 2
1( ) ( 1) ( ) (3)
! ( 1) 2
rr n
nr
rr n
nr
xJ x
r n r
xJ x
r n r
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The explicit relation ship between The explicit relation ship between andand
for integral n isfor integral n is
shown in the following theorems
Theorem 2
Theorem 6
Theorem 1
Theorem 3
Theorem 4
Theorem 5
Theorem 7
J
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Theorem 1Theorem 1
When n is an integer (positive or negative) 2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
( ) ( 1) ( )nn nJ x J x
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Theorem 2Theorem 2
The two independent solutions of Bessel’s
equation may be taken to be
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
( )
cos( ) ( ) ( )( )
sin( )
n
n nn
J x
and
n J x J xY x
n
( )
cos( ) ( ) ( )( )
sin( )
n
n nn
J x
and
n J x J xY x
n
For all values of n.
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Theorem 3Theorem 3
2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
-Generating function for the Bessel functions
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
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Theorem 4Theorem 4
2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
Integral representations for Bessel functions:
1( ) cos(( ) sin ) ( int )nJ x n x d n eger
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Theorem 5Theorem 5
2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
12
1122 1
2112
( )( ) (1 ) ( )
( )
nn ixt
n
xJ x t e dt n
n
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2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
Recurrence Relations
1
1
'1
( ( ))) ( )
( ( ))) ( )
) ( ) ( ) ( )
nnn
n
nnn
n
nn n nx
d x J xi x J x
dx
d x J xii x J x
dx
iii J x J x J x
'1
' 11 12
21 1
) ( ) ( ) ( )
) ( ) { ( ) ( )}
) ( ) ( ) ( )
nn n nx
n n n
nn n nx
iv J x J x J x
v J x J x J x
vi J x J x J x
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2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
graphs of the Bessel functions
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2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
graphs of the Bessel functions
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2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
graphs of the Bessel functions
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Theorem 6Theorem 6
2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
Orthogonally of the Bessel functions
2 212
0
( ) ( ) { ( )}a
an i n j n i ijxJ x J x J x
If i jand are roots of the equation
( ) 0nJ a
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Theorem 7Theorem 7
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
If f(x) is defined in the region
-Bessel Series0 x a
and can be expanded in the form
1
( )i n ii
c J x
Where the i
are the roots of the equation ( ) 0,nJ a
then 0
2 21
2 ( ) ( )
{ ( )}
a
n i
in i
xf x J x dx
ca J a
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2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
problems
1-Use the generating function to prove that
( ) ( ) ( )n r n rr
J x y J x J y
2- Show that
1
0
( )nn
J xdx
x
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2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
Integral equation
Definition(1)
Defintion (2)
Defintion (3)
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2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
An integral equation is an equation in which an unknown function
appears under one or more integral signs.Naturally, in such an equation there
can occur other terms as well .
Integral equation
Definition(1))
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22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
For example
for
, ,a s b a t b for The equation
( ) ( , ) ( ) (1)b
a
f s k s t t dt
2
( ) ( ) ( , ) ( ) (2)
( ) ( , )[ ( )] (3)
b
a
b
a
s f s k s t t dt
s k s t t dt
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Where the function
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
for
( )s
is the unknown function which all the functions are known are integral equation .
These functions may be complex –valued functions of the variables S and t
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2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
An integral equation is called linear if only linear operations are performed function on it upon the unknown function .
The equations (1) and (2) are Linear while (3) is nonlinear.
Integral equation
Definition(2))
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22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
Integral equation
Definition(3))The most general type of linear integral equation is of the form:
( ) ( ) ( ) ( , ) ( ) (4)a
h s s f s k s t t dt Where the upper limit be either variable or fixed.
The functions are known functions, 1 1,f h and k
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While
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
for
( )s is to be determined ;
is called the kernel .
is a nonzero,real or complex, parameter
( , )k s t Is called the Kernel
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2
2 2 22
( ) 0 (1)d y dy
x x x y ydx dx
22 2 2
2( ) 0 (1)
d y dyx x x y ydx dx
1 12 ( ) 2 ( )tx t
nn
e t J x
1 12 ( ) 2 ( )tx t
nn
e t J x
Special casesThe following special cases of
equation (4) are of main interest :
I) Fredholm integral equation
II) Volterra Equations
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I) Fredholm integral equation:
In all Fredholm integral equation of the first kind the upper limit of integration b,say,is fixed.
i) In the Fredholm integral equation of the first kind Thus,( ) 0.h s ( ) ( , ) ( )b
a
f s k s t t dt
( ) ( , ) ( )b
a
f s k s t t dt =0 (5)
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I) Fredholm integral equation:
ii) In the Fredholm integral equation of the second kind,
( ) 1;h s
( ) ( ) ( , ) ( ) (6)b
a
s f s k s t t dt
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I) Fredholm integral equation:
iii) The homogeneous Fredholm integral equation of the second kind is a special case of(ii) above . In this case ( ) 0f s
( ) ( , ) ( ) (7)b
a
s k s t t dt
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II) Volterra Equations II) Volterra Equations
Volterra Equations of the first, homogeneous ,and second kinds are precisely as above except that
b s is the variable upper limit of integration.
Equation (4) itself is called an integral equation of the third kind
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Singular Integral equation:Singular Integral equation:
Definition (4)
When one or both limits of integration become infinite or when the kernel becomes infinite at
one or more points within the range of integration ,the integral equation is
called Singular .
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For example ,the Integral equationsFor example ,the Integral equations
0
( ) ( ) ( ) (8)
1( ) ( ) , 0 1 (9)
( )
s t
s
s f s e t dt
and
f s t dts t
Are singular integral equations.
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Special Kinds of kernelSpecial Kinds of kernel
separable or degenerate kernels
Symmetric kernel
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I) separable or degenerate kernels
A kernel to k(s,t) is called separable or degenerate if it can be expressed as the sum of a finite number of terms each of which is the product of a function s only and a function of only ; that is,
1
( , ) ( ) ( ) (10)n
i ii
k s t a s b t
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II) Symmetric kernel
A complex-valued function K(s,t) is called
symmetric (or Hermitian) if *( , ) ( , ),k s t k t s
where the asterisk denotes the complex conjugate.For a real kernel, this coincides with definition
( , ) ( , )k s t k t s
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Eigen values and eigen Eigen values and eigen functions functions
Eigen values and eigen Eigen values and eigen functions functions
If we write the homogeneous Fredholm equation as
We have the classical eigen value or characteristic value problem; is the eigen value and is the corresponding eigen function or characteristic function.
( )t
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Relationship between linear differential equations and Volterra integral
equation:
Relationship between linear differential equations and Volterra integral
equation:
The solution of the linear differential equation
With continuous coefficients ( ) ( 1,2,3....., )ia x i n
given the initial conditions ' 1
0 1 1(0) , (0) ,........, (0) (12)nny c y c y c
may be reduced to a solution of some Volterra integral equation of the second kind
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From this hypothesis and some mathematical treatment we reach to
)13()(),()()(0
dtttsksfsx
where
1 2
1 1 1 2 0 2
( , ) [ ( ) ( )( )]
( ) ( ) ( ) ( ) ( )
k s t a s a s s t
f s F s c a s c sa s c a s
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Methods of solutionMethods of solution
We shall explain some methods for solving linear integral equations ;
These methods are :
1- Analytical methods2- Numerical methods
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Analytical methods for solving Volterra integral equation:
Resolvent kernel of Volterra integral equation. The method of successive approximation.
using Laplace Transform.
Solution of integro- differential equations with the aid of the Laplace transformation.
( 1)n
x
( 1)n
t
in
in
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( , )k x t
( 1)n
x
( 1)n
t
I)If the kernel is a polynomial of degree
in
i) If the kernel has the general form k(x,t).
ii) If the kernel is a polynomial of degree (n-1) in x or (n-1) in t.
iii) the kernel is dependent on the difference of the arguments.
in
Resolvent kernel of Volterra Resolvent kernel of Volterra integral equation integral equation
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( , )k x t
( 1)n
x
( 1)n
t
in
in
In the three cases above we shall begin with Volterra integral equation of the form
And after some manipulation we shall have ( , ; )R x t
Where is called the resolvent kernel .( , ; )R x t
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The method of successiveThe method of successive approximationapproximation
0 ( )x
( ),x
1( ).x
{ ( )}, 0,1,2,3,.....n x n
we got
, where
0 ( )x
( ),x
1( ).x
Suppose we have a Volterra type integral equation (14).Take some function Suppose we have a Volterra type integral equation (14).
Take some function continuous in [0,a]
into the right side of (14 ) in place of we got
Continuing the process, we obtain a sequence of
Functions where,
0 ( )x
( ),x 1( ).x
{ ( )}, 0,1,2,3,.....n x n
1
0
( ) ( ) ( , ) ( )x
n nx f x k x t t dt
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Where the sequence ( , )k x t
( 1)n
x
( 1)n
t
in
in
{ ( )}n x converges as n
to the solution of the integral equation (14) ( )x
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Using Laplace transformUsing Laplace transform
0 ( )x
( ),x
1( ).xwe got
, where
0 ( )x
( ),x
1( ).x
The Laplace transformation may be employed in the solution of systems of Volterra integral equations of the type
xs
i ijj=1 0
(x)=f (x)+ k (x-t) (t)dt ( 1,2,3,...., ) (15)i j i s
( ), ( )ij ik x t f xWhere are known
continuous functions having Laplace transforms .
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0 ( )x
( ),x
1( ).xwe got
0 ( )x
( ),x
1( ).x
Taking the Laplace transform of both sides of (15) we get :
1
( ) ( ) ( ) ( ) ( 1,2,....., ) (16)s
i i ij Jj
p F p k p p i s
This is asymptotic of linear algebraic equations in
( )i p Solving it ,we find ( )i p
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Analytical methods for Analytical methods for solving Fredholm integral equation:solving Fredholm integral equation:
The method of Fredholm Determinants
Integral Equation with degenerate kernels
( , )k x t
( 1)n
( 1)n
t
I)If the kernel is a polynomial of degree
in
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The method of Fredholm Determinants The method of Fredholm Determinants
0 ( )x
( ),x
1( ).xwe got
0 ( )x
( ),x
1( ).x
The solution of the Fredholm equation of the second kind
is given by the formula
( ) ( , ) ( ) ( ) (17)b
a
x k x t t dt f x
( ) ( ) ( , ; ) ( ) (18)b
a
x f x R x t f t dt
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Where the function
( , )k x t
( 1)n
x
( 1)n
t
in
in
is called
the Fredholm resolvent kernel of equation (17) and defined by the equation
( , ; )R x t
( , ; )( , ; )
( )
D x tR x t
D
Provided the Here,
are power series in :
( ) 0D ( , ; ) ( )D x t and D N
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( , )k x t
( 1)n
x
( 1)n
t
in
in
1
1
( 1)( ) 1
!
( , ) ( , ) ( , ) ( , )
nn
nn
b
n n n
a
D cn
where
B x t c k x t n k x s B s t ds
1
0 0
( , )
1, ( , ) ( , )
b
n n
a
c B s s ds
c B x t k x t
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Integral Equation with Integral Equation with degenerate kernelsdegenerate kernels
0 ( )x
( ),x
1( ).xwe got
0 ( )x
( ),x
1( ).x
The kernel 1
( , ) ( ) ( ) (20)n
k kk
k x t a x b t
The integral equation (17) with degenerate kernel (20) has the form
1
( ) [ ( ) ( )] ( ) ( ) (21)n
k kk
x a x b t t dt f x
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( , )k x t
( 1)n
x
t
in
in
After some manipulation ,it has the form
( 1,2,...., ) (22)m km k mc a c f m n
Where
( ) ( ) ,
( ) ( ) ,
( ) ( )
b
km k m
a
b
m m
a
b
k k
a
a a t b t dt
f b t f t dt
c b t t dt
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Numerical methods for Numerical methods for solving Volterra integral equation:solving Volterra integral equation:
using the trapezoidal rule
( 1)n
x
( 1)n
t
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the trapezoidal rule the trapezoidal rule
0 ( )x
( ),x
1( ).xwe got
0 ( )x
( ),x
1( ).x
Consider the nonhomogeneous Volterra integral equation of the second kind
( ) ( , ) ( ) ( ) (23)x
a
x k x t t dt f x
To apply the trapezoidal rule , let and
( ), 1,nx a
t nn
Define applying the , 1(1)jt a j t j n
trapezoidal rule to the integral of (23) ,we obtain:1
1 10 02 2
1
( ) [ ( , ) ( ) ( , ) ( ) ( , ) ( )] ( ) (24)n
i i n ni
x t k x t t k x t t k x t t f x
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0 ( )x
( ),x
1( ).xwe got
0 ( )x
( ),x
1( ).x
, 1,j n nt x j x x t the integration in (23) is over
, ,t a t x Thus for we take t x
( , ) 0 ,i j j ik x t for t x
the equation (24) can be written in the form :
0 0
11 1
0 02 21
( ) ( )
( ) ( ) [ ( , ) ( , ) ( , ) ], 1, 2,..., ; (25)n
i i i i j j i j j j ij
x f x
x f x t k x t k x t k x t i n t x
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
The system of equation in (25) can be written in a more compact form as
0 0
11 1
,0 02 21
[ ) ], 1, 2,..., ; ( , ), , (26)n
i i i i j j i j j ij i jj
f
f t k k k i n k k x t j i
After some manipulation , we obtain
10 112
0 1 22 2
1 0 0 0 0
(1 ) 0 0
(1 )
t
t tn n n nn
k tk
k tk tk k
0 0
1 1 (27)
n n
f
f
f
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
By solving the system (27) we find
0 1 2 2 1, , ,......, , , .n n n
Which is an approximatetion of the solution of (23)
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Numerical methods for Numerical methods for solving Fredholmsolving Fredholm integral equation:integral equation:
of the second kindof the second kind
The approximate method that we will discuss here for solving Fredholm equation of the second kind:
( 1)n
x
( 1)n
t
( ) ( ) ( , ) ( ) (28)b
a
x f x k x t t dt
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
Are based on approximating the solution
of (28) by a partial sum:
1
( ) ( ) (29)N
N i ii
S x c x
( )x
On the internal (a,b).If we substitute from (29)
into (28) for there will be an error
Of N linearly independent functions 1 2 3 1, , ,....., ,n n
( )x
1 2 3 1( , , , ,....., , )N Nx c c c c c
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
x
Involved which depends on x and on the way
the coefficients are chosen 1 2 3 2 1, , ,......., , ,N N Nc c c c c c
1 2 3 1( ) ( ) ( , ) ( ) ( , , , ,....., , ) (30)b
N N N N
a
S x f x k x t S t dt x c c c c c
Our main goal is how we can find or impose N conditions of the approximate solution (30).
1 2 3 1, , ,....., ,N Nc c c c c
1 2 3 1, , ,....., ,N Nc c c c c
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The Galerkin approximate method The Galerkin approximate method
0 ( )x
( ),x
1( ).xwe got
0 ( )x
( ),x
1( ).x
In this method the N conditions are established for the determination of the N coefficients in (29)
By making of (30) 1 2 3 1( , , , ,....., , )N Nx c c c c c
orthogonal to N given linearly independent Functions on the interval (a,b).
1 2 3( ), ( ), ( ),......., ( )Nx x x x
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
x1 2 3 1, , ,....., ,N Nc c c c c
We will use the definition of orthogonality on
1 2 3 1( , , , ,....., , )N Nx c c c c c in (30) , Then these N
conditions become
1 2 3 10 ( ) ( , , , ,....., , )b
j N N
a
x x c c c c c ds
0 ( )[ ( ) ( ) ( , ) ( ) ] ( 1,2,3,...., )b b
j N N
a a
x S x f x k x t S t dt ds j N
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
1 2 3 1, , ,....., ,N Nc c c c c
After some manipulation ,we obtain :
1 1
( ){ ( ) ( , ) ( ) } ( ) ( ) , 1,2,3,...., (31)b b bN N
j i i i i ji ia a a
x c x k x t c t dt ds x x dx j N
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Differential EquationsDifferential EquationsDifferential EquationsDifferential Equations
1- Power series solutions about an ordinary pointthis will not be discussed here because it has been taken in the past {Bs.C}
2-Solutions for singular points; the method of Frobineous
3- Bessel’s equation and Bessel Functions
Series solutions of linear differential equations
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The method of FrobineousThe method of Frobineous
0 ( )x
( ),x
1( ).xwe got
0 ( )x
( ),x
1( ).x
We consider the homogeneous linear differential equation
2
0 1 22( ) ( ) ( ) 0 (1)d y dy
a x a x a x ydx dx
And we assume that 0x
is singular point of (1) under certain conditions we are justified in assuming a solution of the form
0 00
( ) (2)r n
nn
y x x c x x
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
Where r is a certain (real or complex ) constsnt.Again,we write the differential equation (1)
in the equivalent normalized form2
1 22( ) ( ) 0 (3)
d y dyp x p x y
dx dx
where
Outline of the method of Frobenius:
1- Let a regular singular point of the differential Equation (1), seek solutions valid in some interval
0x
00 ,x x R
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
and assume a solution
0 00
( ) ( )r nn
n
y x x c x x
Where we write the solution in the 0 0c
00
( ) (4)n rn
n
y c x x
2- Assuming term by term differentiation of (4)Is valid ,we obtain
10
0
( ) ( ) (5)n rn
n
dyn r c x x
dx
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
and
Now we substitute the series (4),(5) and (6) for y and its derivatives, respectively ,into the differential equation (1)
3- Now we proceed to simplify the resulting expression So that it takes the form
22
020
( )( 1) ( ) (6)n rn
n
d yn r n r c x x
dx
10 0 1 0( ) ( ) .... 0 (7)r k r kk x x k x x
k
( 0,1,2,.....)ik i
r
nc
are functions of
Where K is a certain integer and the coefficients
( 0,1,2,.....)ik i are functions of r and certain of the coefficients of the solution of (4)nc
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
x
00 ,x x R
we must set
4- In order that (7) be valid for all X in the deleted interval we must set 00 ,x x R
0 1 2 ...... 0nk k k k
5- Upon equating to zero the coefficient of the
lowest power of , we obtain
a quadratic equation in r called the indicial equation of the differential equation (1) .The two roots of this quadratic equation in r , called the indicial equation of the differential equation (1)
0k
r k 0( )x x
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
x
00 ,x x R
The two roots of this quadratic equation in r , called the indicial equation of the differential equation (1).The two roots of this quadratic equation are often called the exponents of the differential equation (1) and are the only possible values for the constant r in the assumed solution (4) .Thus at this stage the unknown constant is determined .We denote the roots of the indicial equation by where Here denotes the real part of and of
course if is real ,then is simplify it self.
1 2r and r 1 2Re( ) Re( ).r r
Re( )jr ( 1,2)jr j
jr Re( )jr jr
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
x
00 ,x x R
6- Now we equateto zero the remaining coefficients in (7) ,we are thus led to
a set of conditions, involving the constants r which must be satisfied by the various coefficients in the series (4).
1 2 3 4, , , ......k k k k
nc
1r for r
nc
nc
1r r
1r
2r
1r
and
are real and unequal , then
is the larger root.
7- We now substitute the root into the conditions obtained is step 6 , and then choose the to satisfy these conditions . If the are so chosen , the resulting series (4) with
is a solution of the desired form. Note that if and are real and unequal , then is the larger root.
1r for r
nc nc
1r r
1r2r
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0 ( )x
( ),x
1( ).x
0 ( )x
( ),x
1( ).x
x
00 ,x x R
1r for r
nc
nc
1r r
1r
2r
1r
and
are real and unequal , then
is the larger root.
8- if ,we may repeat the procedure of step (7) using the root instead of In this way a second solution of the desired form (4) may be obtained . Note that if and are real and unequal , then is the smaller root . However , in the case in which and real and unequal , the second solution of the desired form (4) obtained in this step may not be linearly independent of the solution obtained in step (7) . also , in the case which are real and equal , the solution obtained in the step is clearly identical with the one obtained in step (7)
1 2r r2r 1r
1r 2r
2r
2r1r
1 2r and r
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I hope that the presentation
is useful