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Chapter 2 Theory of First Order Differential Equations Shurong Sun University of Jinan Semester 1, 2011-2012

Chapter 2 Theory of First Order Differential Equations

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Chapter 2 Theory of First Order Differential Equations. Shurong Sun University of Jinan Semester 1, 2011-2012. 1 Existence-uniqueness theorem ( Picard’s Method of Successive Approximations ). Consider the initial-value problem. (1). - PowerPoint PPT Presentation

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Page 1: Chapter 2 Theory of First Order Differential Equations

Chapter 2 Theory of First Order Differential

Equations

Shurong Sun

University of Jinan

Semester 1, 2011-2012

Page 2: Chapter 2 Theory of First Order Differential Equations

Consider the initial-value problem

0 0( , ), ( )dy

f t y y t ydt (1)

Q1. How to know that the IVP (1) actually has a solution if we can’t exhibit it?

1 Existence-uniqueness theorem (Picard’s Method of Successive Approximations)

2 2 , (0) 0;dy

t y ydt

Q2. How do we know that there is only one solution y(t) of (1)?

2 , (0) 0.dy

y ydt

2( ) ,( , 0.)

0,

t c t cy c

t c

Page 3: Chapter 2 Theory of First Order Differential Equations

The short answer to the question, how do you know the equation has a solution, is ‘Picard iteration’.

Iteration means to do something over and over.

Picard’s Existence and Uniqueness Theorem is one of the most important theorems in ODE!

Why is Picard’s Theorem so important?

( ) 0f x ( )x g x 0take x 1 0( )x g x

1( )n nx g x If *, nx x n * ( *).x g x

Page 4: Chapter 2 Theory of First Order Differential Equations

00 ( , ( )) .

t

ty y f s y s ds

(ii) Pick a function 0( )y t

Pick 0 0( ) .y t y

Define 1( ) byy t

01 0 0( ) ( , ( )) .

t

ty t y f s y s ds

Then we iterate: define

02 0 1( ) ( , ( )) .

t

ty t y f s y s ds

0 0( ( , ), ( ) )dy

f t y y t ydt

satisfying the initial condition.

(i) Rewrite the differential equation as an integral equation:

Page 5: Chapter 2 Theory of First Order Differential Equations

and having defined 1( ), , ( )ny t y t define

01 0( ) ( , ( )) .

t

n nty t y f s y s ds

This gives a sequence of functions

1 2( ), ( ),y t y t

The solution is ( ) lim ( ),nny t y t

when Picard

Intuitively, is the solution since( )y t

iteration works.

Picard iteration

Page 6: Chapter 2 Theory of First Order Differential Equations

01 0( ) ( , ( ))

t

n nty t y f s y s ds

But then 0 0( ) .y t yand( , )dy

f t ydt

00lim ( ) lim ( , ( ))

t

n ntn ny t y f s y s ds

00( ) ( , ( ))

t

ty t y f s y s ds

Page 7: Chapter 2 Theory of First Order Differential Equations

Remark: Was that a foolproof proof?

00lim ( ) lim ( , ( ))

t

n ntn ny t y f s y s ds

Almost, but the formula

is called ‘taking the limit under the integral sign’ and it is not always correct.

We need to add some further conditions on f to make it work. But basically this is the idea.

00 lim ( , ( ))

t

nt ny f s y s ds

Page 8: Chapter 2 Theory of First Order Differential Equations

Theorem 1.1 (Existence and uniqueness for the Cauchy problem)

and suppose that

0 0{( , ) :| | ,| | }A t y t t a y y b

:f A R• is continuous,

Then the Cauchy problem

0 0( , ), ( )dy

f t y y t ydt (1)

has a unique solution on0 0[ , ],t h t h

Let

where

( , )min( , ) with max | ( , ) | .

t y A

bh a M f t y

M

• satisfies a Lipschitz condition with respect to y.

Page 9: Chapter 2 Theory of First Order Differential Equations

0 0( , )t y

0t a0t a

0y b

0y b

min{ , }b

h a aM

MM

Page 10: Chapter 2 Theory of First Order Differential Equations

0 0( , )t y0t a0t a

0y b

0y b

min{ , }b b

h aM M

MM

Page 11: Chapter 2 Theory of First Order Differential Equations

Proof of the Theorem

We will prove the theorem in five steps:

(i) Show that the initial value problem

0 0( , ), ( )dy

f t y y t ydt

is equivalent to the integral equation

00 ( , ( )) .

t

ty y f s y s ds

(1)

(2)

Page 12: Chapter 2 Theory of First Order Differential Equations

(ii) Set up a sequence of Picard iteration and show that they are well defined.

(iii) Show that our sequence of Picard iteration converges uniformly.

(iv) Show that the function to which our sequence converges is a solution to the IVP.

(v) Show that this solution is unique.

Page 13: Chapter 2 Theory of First Order Differential Equations

(i) The initial-value problem

0 0( , ), ( )dy

f t y y t ydt (1)

Specifically, if y(t) satisfies (1), then

is equivalent to the integral equation

00( ) ( , ( )) .

t

ty t y f s y s ds (2)

0 0

( )( , ( )) .

t t

t t

dy sds f s y s ds

ds

Hence 0

0( ) ( , ( )) .t

ty t y f s y s ds (2)

Page 14: Chapter 2 Theory of First Order Differential Equations

Conversely, if y(t) is continuous and satisfies (2),

( , ).dy

f t ydt

Moreover, 0 0( ) .y t y

Therefore, y(t) is a solution of (1) if, and only if, it is a continuous solution of (2).

then

00( ) ( , ( )) .

t

ty t y f s y s ds

Page 15: Chapter 2 Theory of First Order Differential Equations

(ii) Construction of the approximating sequence

( ).ny tLet us start by guessing a solution 0( )y t of (2).

The simplest possible guess is 0 0( ) .y t y

To check whether 0( )y t is a solution,

01 0 0( ) ( , ( )) .

t

ty t y f s y s ds

we compute

If 1 0( ) ( ),y t y t then 0( ) ( )y t y t is indeed a solution

of (2). 1( )y t as our next guess.If not, then we try

Page 16: Chapter 2 Theory of First Order Differential Equations

To check whether 1( )y t is a solution, we compute

02 0 1( ) ( , ( )) .

t

ty t y f s y s ds

and so on.

In this manner, we define a sequence of functions

1 2( ), ( ), ,y t y t

where 0

1 0( ) ( , ( )) .t

n nty t y f s y s ds (3)

These functions ( )ny t

or Picard iteration,

are called successive approximation,

who first discovered them.

after the French mathematician Picard

Page 17: Chapter 2 Theory of First Order Differential Equations

Define the sequence of Picard iteration as

0

0 0 0

0 1 0

( ) ,| | ,

( ) ( , ( )) ,| | , 1.t

n nt

y t y t t h

y t y f s y s ds t t h n

To ensure that Picard iteration are well defined it is sufficient to ensure that each ( )ny t that is

0 0| ( ) | ,| | .ny t y b t t h (4)

stays within [-b,b],

0;t t0.t t

It’s convenient to assume a similar proof will hold for

Page 18: Chapter 2 Theory of First Order Differential Equations

We prove (4) by induction on n.

Observe first that (4) is obviously true for n=0, since

0 0( ) .y t yNext, we must show that (4) is true for n=j+1 if it is true for n=j.

But this follows immediately, for

0| ( ) | ,jy t y b then

1 0| ( ) |jy t y

0

| ( , ( )) |t

jtf s y s ds

for 0 0 .t t t h

0 0

(| ( ) | | ( ) | )t t

t tf s ds f s ds

0 0

( ( ) ( ) ( ) | ( ) )t t

t tf t g t f s ds g s ds

0( )M t t Mh

0 0 0| ( ) | , .ny t y b t t t h

01 0( ) ( , ( )) .

t

n nty t y f s y s ds

0

| ( , ( )) |t

jtf s y s ds

b

.

Page 19: Chapter 2 Theory of First Order Differential Equations

Clearly, the sequence

0 0[ , ]t t h

(iii) We now show that our sequence of Picard iteration converges uniformly for t in the interval

This is accomplished by writing ( )ny t in the form

0 1 0 1( ) ( ) [ ( ) ( )] [ ( ) ( )]n n ny t y t y t y t y t y t ( )ny t converges

and only if, the infinite series

1 0 1[ ( ) ( )] [ ( ) ( )]n ny t y t y t y t

converges .

if,

Page 20: Chapter 2 Theory of First Order Differential Equations

it suffices

11

| ( ) ( ) | .n nn

y t y t

Observe that

01 1 2| ( ) ( ) | | [ ( , ( )) ( , ( ))] |

t

n n n nty t y t f s y s f s y s ds

0 0 .t t t h (5)

To prove the infinite series converges,

01 2| ( , ( )) ( , ( )) |

t

n ntf s y s f s y s ds

01 2| ( ) ( ) | ,

t

n ntL y s y s ds

to show that

01 0 0 0| ( ) ( ) | | ( , ) | ( )

t

ty t y t f s y ds M t t

Page 21: Chapter 2 Theory of First Order Differential Equations

02 1 1 0| ( ) ( ) | | ( ) ( ) |

t

ty t y t L y s y s ds

20( )

,2

LM t t

00( )

t

tLM s t ds

This, in turn, implies that

03 2 2 1| ( ) ( ) | | ( ) ( ) |

t

ty t y t L y s y s ds

0

22 0( )

2

t

t

s tML ds

2 30( )

.3!

ML t t

Setting n=1 in (5) gives

Page 22: Chapter 2 Theory of First Order Differential Equations

Proceeding inductively, we see that1

01

( )| ( ) ( ) | ,

!

n n

n n

ML t ty t y t

n

0 0for .t t t h

Therefore, for 0 0 ,t t t h

1

1| ( ) ( ) | .!

n n

n n

ML hy t y t

n

Consequently, converges uniformly ( )ny t

on the interval 0 0 ,t t t h since1

.!

n nML h

n

Page 23: Chapter 2 Theory of First Order Differential Equations

We denote the limit of the sequence ( )ny t

(iv) Prove that y(t) satisfies the initial-value problem (1)

We will show that y(t) satisfies the integral equation

0 0[ , ].t t h

00 ( , ( ))

t

ty y f s y s ds

which is continuous on

by y(t),

To this end, recall that the Picard iteration ( )ny t

are defined recursively through the

01 0( ) ( , ( )) .

t

n nty t y f s y s ds

Taking limits of both sides of (6) gives

(6)

00( ) lim ( , ( )) .

t

ntny t y f s y s ds

equation

Page 24: Chapter 2 Theory of First Order Differential Equations

( , ( ))nf s y s converges uniformly

since

0 0| ( , ( )) ( , ( )) | | ( ) ( ) |, .n nf s y s f s y s L y s y s t s t h and ( )ny t

0 0[ , ],t t hon

0 0[ , ].t t h

Note that to f(s,y(s))

converges uniformly to y(t) on

Then one can exchange integral and the limit.

Thus

0 0 0

lim ( , ( )) lim ( , ( )) ( , ( )) ,t t t

n nt t tn nf s y s ds f s y s ds f s y s ds

and y(t) satisfies0

0 ( , ( )) .t

ty y f s y s ds

Page 25: Chapter 2 Theory of First Order Differential Equations

(i) Let z(t) be also a solution of (2). By induction we show that

10( )

| ( ) ( ) | .( 1)!

n n

n

ML t tz t y t

n

We have

00( ) ( ) ( , ( ))

t

tz t y t f s z s ds

and therefore

which (7) holds for n = 0.

0 0| ( ) ( ) | ( )z t y t M t t

(7)

(v) Show that the solution is unique.

Page 26: Chapter 2 Theory of First Order Differential Equations

If (7) holds for n − 1 we have

01| ( ) ( ) | | [ ( , ( )) ( , ( ))] |

t

n ntz t y t f s z s f s y s ds

and this proves1

0( )| ( ) ( ) | .

( 1)!

n n

n

ML t tz t y t

n

0

10( )

!

n nt

t

ML s tL ds

n

10( )

,( 1)!

n nML t t

n

01| ( ) ( ) |

t

ntL z s y s ds

for all .n N

Page 27: Chapter 2 Theory of First Order Differential Equations

Consequently,1

| ( ) ( ) | .( 1)!

n n

n

ML hz t y t

n

This implies that

1

lim 0,( 1)!

n n

n

ML h

n

since

1

0

.( 1)!

n n

n

ML h

n

( )ny t converges uniformly

to z(t) on 0 0 .t t t h

And so 0 0( ) ( ), .y t z t t t t h

Page 28: Chapter 2 Theory of First Order Differential Equations

(v) (ii) It remains to prove uniqueness of the solution. Let y(t) and z(t) be two solutionsof (2). By recurrence we show that

102 ( )

| ( ) ( ) | .( 1)!

k kML t ty t z t

k

We have

0

( ) ( ) [ ( , ( )) ( , ( ))]t

ty t z t f s y s f s z s ds

and therefore

which (7) for k = 0.

0| ( ) ( ) | 2 ( )y t z t M t t

(7)

Page 29: Chapter 2 Theory of First Order Differential Equations

If (7) for k − 1 holds we have

0

| ( ) ( ) | | [ ( , ( )) ( , ( ))] |t

ty t z t f s y s f s z s ds

and this proves1

02 | || ( ) ( ) | .

( 1)!

k kML t ty t z t

k

0

102 ( )

!

k kt

t

ML s tL ds

k

102 ( )

,( 1)!

k kML t t

k

0

| ( ) ( ) |t

tL y s z s ds

for all .k N

Page 30: Chapter 2 Theory of First Order Differential Equations

Consequently,12

| ( ) ( ) | .( 1)!

k kML hy t z t

k

This implies that

12lim 0,

( 1)!

k k

k

ML h

k

since

1

0

2.

( 1)!

k k

k

ML h

k

0 0( ) ( ), .y t z t t t t h

Page 31: Chapter 2 Theory of First Order Differential Equations

Remark: (1) Geometrically, this means the graph

of ( )y t

region shown below.

is constrained to lie in the shaded

Page 32: Chapter 2 Theory of First Order Differential Equations

0 0( , )t y 0t a0t a

0y b

0y b

min{ , }b

h a aM

0 0( )y y M t t 0 0( )y y M t t

Page 33: Chapter 2 Theory of First Order Differential Equations

0 0( , )t y0t a0t a

0y b

0y b

min{ , }b b

h aM M

0 0( )y y M t t 0 0( )y y M t t

Page 34: Chapter 2 Theory of First Order Differential Equations

Remark: (2) Geometrically, this means the graph

is constrained to lie in the shaded( )ny tof

region shown below.

Page 35: Chapter 2 Theory of First Order Differential Equations

(3) If f

y

is continuous in the rectangle A ,

then f satisfies a Lipschitz condition,

1 2 1 2 1 2

1 2

| ( , ) ( , ) | | ( ) | | |

for all ( , ), ( , ) ,

ff t y f t y y y L y y

y

t y t y A

where

( , )max .t y A

fL

y

Note that f satisfies a Lipschitz condition

f

y

is continuous.

For example: f(t,y)=|y|.

since

Page 36: Chapter 2 Theory of First Order Differential Equations

Corollary : Let f and f

y

be continuous in the

rectangle0 0{( , ) :| | ,| | }.A t y t t a y y b

Compute ( , )max | ( , ) | and set min( , ) .t y A

bM f t y h a

M

Then the initial problem

0 0( , ), ( )dy

f t y y t ydt

has a unique solution y(t) on the interval 0 0[ , ].t h t h

Page 37: Chapter 2 Theory of First Order Differential Equations

Show that the solution y(t) of the initial-value problem

exists for and in this interval,

22 , (0) 0ydyt e y

dt

1 1,

2 2t | ( ) | 1.y t

Solution: Let 1

{( , ) :| | ,| | 1}.2

A t y t y

Computing 22

( , )

5max ,

4y

t y AM t e

we see that y(t) exists for 1| | ,

2t h and in this

| ( ) | 1.y t

Example 1.1

1 1 1min( , ) ,

52 24

h

interval,

Page 38: Chapter 2 Theory of First Order Differential Equations

Remark (4) The initial value problem (IVP)

where

has a unique solution valid on [a, b].

0 0, [ , ], [ , ]p q C a b t a b and y R

0 0( ) ( ), ( ) ,dy

p t y q t y t ydt

Page 39: Chapter 2 Theory of First Order Differential Equations

Proof

The unique solution is to the IVP

is

0 0( ) ( ), ( )dy

p t y q t y t ydt

0 0

0

( ) ( )

0( ( ) ),t u

x xP s ds P s dst

xy e q u e du y

[ , ].t a b

(Method I)

Page 40: Chapter 2 Theory of First Order Differential Equations

Method II Successive approximation

(i) Show that the initial value problem

0 0( ) ( ), ( )dy

p t y q t y t ydt

is equivalent to the integral equation

00( ) [ ( ) ( ) ( )] .

t

ty t y p s y s q s ds

(1)

(2)

Specifically, y(t) is a solution of (1) on [a,b] if, and only if, it is a continuous solution of (2) on [a,b].

Page 41: Chapter 2 Theory of First Order Differential Equations

(ii) Construction of the approximating sequence

0

0 0

0 1

( ) ,

( ) [ ( ) ( ) ( )] , 1.t

n nt

y t y

y t y p s y s q s ds n

(iii) Show that the sequence of Picard iteration

converges uniformly on the interval

{ ( )}ny t

[ , ];a b

Then

are well defined on [a,b] for all ( )ny t 0;n

and only if, the infinite series

1 0 1[ ( ) ( )] [ ( ) ( )]n ny t y t y t y t

{ ( )}ny t converges if,

converges .

Page 42: Chapter 2 Theory of First Order Differential Equations

Take 0[ , ]

max | ( ) ( ) |,x a b

M p x y q x

1 10

1

( )| ( ) ( ) | , [ , ], 1.

! !

n n n n

n n

ML t t ML hy t y t t a b n

n n

Then

[ , ]max | ( ) | .x a b

L p x

(iv) Show that the limit of the sequence { ( )}ny t

is a continuous solution to the integral equation (2) on [a,b].

(v) Show that this solution is unique.

[ , ]max | ( ) ( ) ( ) | .x a b

M p x z s q x

Take1 1

0( ) ( )| ( ) ( ) | , 0.

( 1)! ( 1)!

n n n n

n

ML t t ML b az t y t n

n n

Then

Page 43: Chapter 2 Theory of First Order Differential Equations

Theorem 1.2 (Peano 1890)

and suppose that

0 0{( , ) :| | ,| | }A t y t t a y y b

:f A R is continuous with

Then the Cauchy problem

0 0( , ), ( )dy

f t y y t ydt (1)

has a solution on 0 0[ , ].t h t h

Let

( , )max | ( , ) | .t y A

M f t y

Set min( , ) .b

h aM

Page 44: Chapter 2 Theory of First Order Differential Equations

The method of Picard iteration not only give the solution but also found functions which approximate it well, i.e. Let y(t) be the exact solution of the IVP

Estimates of error and approximate calculation

00 1 0 0( ) ( , ( )) , ( ) .

t

n nty t y f s y s ds y t y

0 0( , ), ( )dy

f t y y t ydt

and the Picard scheme for solving this is

Page 45: Chapter 2 Theory of First Order Differential Equations

If we make in approximating the solution y(t) by

1

| ( ) ( ) | .( 1)!

n n

n

ML hy t y t

n

( ),ny t then the error

is called the nth approximate solution to the( )ny t

IVP.

Page 46: Chapter 2 Theory of First Order Differential Equations

Example1.2 Let

(i) Determine the interval of existence that the Existence Theorem predicts for the solution y(x) of the initial-value problem

2 2dyx y

dx

(ii) Determine an approximate solution of the IVP above such that the error is less than 0.05.

(0) 0y

2 2dyx y

dx , ( , ) :[ 1,1] [ 1,1].x y R

Page 47: Chapter 2 Theory of First Order Differential Equations

Solution: Since , ( ),yf f C R the existence and

From the Existence Theorem, 2 2dyx y

dx (0) 0y

has a unique solution on [-h,h].

Here ( , )max | ( , ) | 2,x y R

M f x y

uniqueness theorem holds.

1 1min{ , } min{1, } .

2 2

bh a

M

Thus, the interval of solution is 1 1

[ , ].2 2

Page 48: Chapter 2 Theory of First Order Differential Equations

2L

1| ( ) ( ) |( 1)!

nn

n

MLx x h

n

11 1

( ) 0.05( 1)! ( 1)!

nMLh

L n n

we can take

| | | 2 | 2,( , ) ,yf y x y R Since

Take then

1

( 1)!n

1 1 10.05

4! 24 20 .

3,n

Page 49: Chapter 2 Theory of First Order Differential Equations

The successive approximates are:

0 ( ) 0x 3

2 21 00( ) [ ( )]

3

x xx x x dx 3 7

2 22 10( ) [ ( )]

3 63

x x xx x x dx

3( )x is the approximate solution desired,

6 10 142 2 2

3 20

2( ) [ ( )] ( )

9 189 3969

x x x xx x x dx x dx

3 7 11 152

3 63 2079 59535

x x x x

3

1 1| ( ) ( ) | 0.05, [ , ].

2 2x x x

Page 50: Chapter 2 Theory of First Order Differential Equations

Example 1.3 The initial value problem

, (0) 1y y y is equivalent to solving the integral equation

01 ( ) .

xy y t dt

Let 0( ) 1.y x We obtain

1 00( ) 1 ( ) 1 ,

xy x y t dt x

2

2 10( ) 1 ( ) 1 ,

2

x xy x y t dt x

100

( 1), ( ) 1 ( ) ,

!

i inx

n ni

xy x y t dt

i

Page 51: Chapter 2 Theory of First Order Differential Equations

Recalling Taylor’s series expansion of

100

( 1), ( ) 1 ( ) ,

!

i inx

n ni

xy x y t dt

i

,xe

The function

we see that

lim ( ) .xnn

y x e

xy e the given initial value problem in R.

is indeed the solution of

Page 52: Chapter 2 Theory of First Order Differential Equations

2. Continuation of solutions

So far we only considered local solutions,

0 0( , ).t y

To extend the solution we solve the Cauchy problem locally, say from

0 0tot t hcontinue the solution by solving the Cauchy problem

( , )dy

f t ydt

with new initial condition 0( ).y t h

(1)

and then we can try to

which are defined in a neighborhood of

i.e. solutions

0 0( , ( ))t h y t h

0 0( , )t y .

0t h 0t h

.

Page 53: Chapter 2 Theory of First Order Differential Equations

In order to do this we should be able to solve it locally everywhere and we will assume that f satisfy a local Lipschitz condition.

Definition A function f(t,y) (where U is an open set of R×R) satisfies a local Lipschitz condition

0 0( , )t y U V U

Remark: If the function f is of class 1C

if for anythere exist a neighborhood

f satisfies a Lipschitz condition on V.

such that

satisfies a local Lipschitz condition.

in U, then it

Page 54: Chapter 2 Theory of First Order Differential Equations

Theorem 2.1 (Theorem on local solvability)

If U is open and ( )f C U

Lipschitz condition in U,

satisfies a local

0 0( , ) ;t y U i.e., there is a neighborhood I of

0t such that exactly one solution exists in I.

problem (1) is locally uniquely solvable for

then the initial value

Page 55: Chapter 2 Theory of First Order Differential Equations

0 0( , )P t yQ

0t

0y

O t

y

0 1t h 0 1t h

M

N

S0 1( )y t h

U

0 1 2t h h

0 1 2t h h

0 1 0 1MQ : ( ),y y t t h t t h

0 1 2 0 1 2NS : ( ),z z t t h h t t h h

0 1 0 1

0 1 0 1 2

( ),MS : ( )

( ),

y t t h t t ht

z t t h t t h h

0 1 0 1

0 1 2 0 1

( ) ( ),

( ) ( ),

y t h z t h

z t y t t h h t t h

Page 56: Chapter 2 Theory of First Order Differential Equations

Consider the differential equation

( , )dy

f t ydt (1)

If y(t) is a solution of (1) defined on an interval I, we say that z(t) is a continuation or extension of y(t) if z(t) is itself a solution of (1) defined on an interval J which properly contains I and z restricted to I equals y .

A solution is non-continuable or saturated if no such extension exists; i.e., I is the maximal interval on which a solution to (1) exists.

Page 57: Chapter 2 Theory of First Order Differential Equations

Lemma 2.1Let U R R :f U R

0 0( , )t y U

max 0( , ), withI t

such that (i) the Cauchy problem

0 0( , ), ( )dy

f t y y t ydt

Lipschitz condition. be an open set and assume that

is continuous and satisfies a localThen for any there exists an open interval

has a unique solution y on max .I

(2) If :z I R is a solution of (1), then max ,I I

(1)

and | .Iz y

Page 58: Chapter 2 Theory of First Order Differential Equations

Proof: (a) Let : , :y I R z J R

of the Cauchy problem with 0 , .t I Jy(t) = z(t) .t I J

be two solutions

Then

Suppose it is not true, 1 such thatt

1 1( ) ( ).y t z tthere is point

Consider the first point where the solutions separate.

The local existence theorem 2.1 shows that it is impossible.

0 0( , )t y

Page 59: Chapter 2 Theory of First Order Differential Equations

(b)

max 0{ is an open interval, t , there exists a solution

of IVP (1) on }.

I I I

I

This interval is open and we can define the solution onmax as follows:I

maxif , then there exists where the Cauchy

problem has a solution and we can define ( ).

t I I

y t

maxThe part (a) shows that ( ) is uniquely defined on .y t I

Define

Page 60: Chapter 2 Theory of First Order Differential Equations

Theorem 2.2

:f U R

( , )dy

f t ydt can be extended to

Let U R R be an open set and assume that is continuous and satisfies a local Lipschitz condition.Then every solution of

the left and to the right up to the boundary of U.

Page 61: Chapter 2 Theory of First Order Differential Equations

right in an interval 0t t b ( is allowed),band one of the following cases applies:(i) ;b the solution exists for all

0 .t t(ii) and lim sup | ( ) | ;

t bb t

the solution “becomes infinite”.(iii) and , (( , ( )), ) 0, .b t t U t b

Remark: solution can be extended to the right

up to the boundary of U means that

exists to the

where (( , ), )t y U denotes the distance from the point (t,y) to the boundary of U.

If U is a bounded region, then (iii) is the only case.

Page 62: Chapter 2 Theory of First Order Differential Equations

exists to the

0a t t ( is allowed),a and one of the following cases applies:

(i) ;a the solution exists for all 0 .t t

(ii) lim sup | ( ) | ;t a

a and t

the solution “becomes infinite”.(iii) lim (( , ( ), ) 0.

t aa and t t U

can be extended to the left up to

the boundary of means that

solution

U

left in an interval

If U is a bounded region, then (iii) is the only case.

Page 63: Chapter 2 Theory of First Order Differential Equations

Determine the maximal intervals on which the solutions to the differential equation

passing through (0,0) and (ln2,-3) exist.

Example 1

Solution: The function2 1

( , )2

yf t y

is defined on

the whole ty-plane and satisfies the conditions of existence Theorem and continuation theorem.

2 1

2

dy y

dt

Page 64: Chapter 2 Theory of First Order Differential Equations

The general solution to the given DE is

Thus the solution passing through (0,0) is

So the maximal interval is

1

1

t

t

cey

ce

1

1

t

t

ey

e

.t

Page 65: Chapter 2 Theory of First Order Differential Equations

The solution passing through (ln2,-3) is

Hence, the maximal interval of this solution is

The domain of this solution is ( ,0) (0, ).

Note that 0 ln 2 and , as 0 .y t

1

1

t

t

ey

e

0 .t

Page 66: Chapter 2 Theory of First Order Differential Equations

tO

y

1

1

(ln 2, 3)

Page 67: Chapter 2 Theory of First Order Differential Equations

Determine the maximal intervals on which the solutions to the IVP exists.

Example 2

Solution: The function1 ln t is defined on

the right-half-plane t>0 and the existence Theorem and continuation theorem hold.

1 ln , (1) 0dy

t ydt

The solution to the IVP is

The solution is well-defined, continuous on t>0, and

So the maximal interval is

ln 0 0.y t t as t (0, ).

ln .y t t

Page 68: Chapter 2 Theory of First Order Differential Equations

Example 3: Prove that for any 0 0and | |t R y a

The solution to the IVP2 2

0 0( ) ( , ), ( )dy

y a f t y y t ydt

exists on 2( , ), where , ( ).yf f C R

Proof: The function

the whole ty-plane and satisfies the conditions of existence Theorem and continuation theorem.

2 2( ) ( , )y a f t y is defined on

It is easy to see that y aDE.

are solutions to the given

Page 69: Chapter 2 Theory of First Order Differential Equations

From the continuation theorem, the solution to 2 2

0 0( ) ( , ), ( )dy

y a f t y y t ydt

the solution can not pass through .y aSo it can only be extended to the left and to the right

y a

y a

0 0( , )t yt

infinitely.

moves away from the origin, but from existence theorem,

Page 70: Chapter 2 Theory of First Order Differential Equations

Let and let us assume that

: is continuous, bounded, and

satisfies a local Lipschitz condition.

Then every solution of ( , )

can be extended to (- , ).

U R R

f U R

y f t y

Remark:

0 0( , )t y

0 0( )y y M t t

0 0( )y y M t t

Page 71: Chapter 2 Theory of First Order Differential Equations

Homework:

1. Determine the maximal intervals on which the solutions to the differential equation

passing through (1,1) and (3,-1) exist.

2dyy

dt

Page 72: Chapter 2 Theory of First Order Differential Equations

2. Prove that for any

The solution to the IVP

0 02 2

( 1), ( )

1

dy y yy t y

dt t y

exists on ( , ).

0 00 1t R and y

Page 73: Chapter 2 Theory of First Order Differential Equations

3 Dependence on initial conditions and parameters

The first-order equation y y has the solution0

0 0 0( ) through the point ( , ).t tt y e t y

(1) Continuous dependence on initial conditions

We first investigate the continuous dependence of the solution 0 0 0 0( , , ) on ( , ).y t t y t y

Consider the IVP

0 0( , ), ( ) .dy

f t y y t ydt

Page 74: Chapter 2 Theory of First Order Differential Equations

Let : ( an open set of ) be

continuous and satisfy a local Lipschitz

condition. Then for any bounded closed

region there exists 0 such that

| ( , ) - ( , ) | | - |, for all

( , ),

f U R U R R

K U L

f t y f t x L x y

t x

( , ) .t y K

Lemma 3.1

Page 75: Chapter 2 Theory of First Order Differential Equations

Proof:

( , ) and ( , ) such thatn n n nt x t y

| ( , ) ( , ) | | | .n n n n n nf t x f t y n x y

By Bolzano-Weierstrass, the sequence ( , )n nt y

accumulation point (t, y). By assumption the function

Since f is bounded on K with( , )max | ( , ) |t y K

M f t y

(1)

has an

Let us assume the contrary. Then there

exist sequences

f(t, y) satisfies a Lipschitz condition in a neighborhood V of (t, y).

it follows from (1) that 2| | .n n

Mx y

n

exists infinitely many indices n such that( , ) , ( , )n n n nt x t y V

Then (1) contradicts the Lipschitz condition on V .

Therefore there

Page 76: Chapter 2 Theory of First Order Differential Equations

Lemma 3.2 (Gronwall inequality) Suppose that g(t) is a continuous function with ( ) 0g t

Then we have0

0( ) ( ) , [ , ].t

tg t a b g s ds t t T

0( )0( ) , [ , ].b t tg t ae t t T

that there exits constants 0, 0a b such that

and

Page 77: Chapter 2 Theory of First Order Differential Equations

Proof: Then

and

Therefore

or, equivalently,

0

( ) ( ) .t

tG t a b g s ds

0( ) ( ), [ , ]g t G t t t T

0( ) ( ), [ , ].G t bg t t t T

Set

00 0( ) ( ) 0, [ , ].btbte G t e G t t t T

0

( ) ( )t

tg t a b g s ds

0( ) ( ), [ , ]G t bG t t t T

0( ) ( ), [ , ]bt bte G t be G t t t T

that is0[ ( )] 0, [ , ].bte G t t t T

Hence

or

which implies that

0 0( ) ( )0 0( ) ( ) , [ , ]b t t b t tG t G t e ae t t T

0( )0( ) , [ , ].b t tg t ae t t T

Page 78: Chapter 2 Theory of First Order Differential Equations

Assume that : ( an open set of ) is

continuous and satisfy a local Lipschitz condition.

f U R U R R Theorem 3.1

0 0

00 0 0 0 0

0, a neighborhood ( , , ) of ( , ),s.t.

ˆ ˆ ˆ| ( , , ) ( , , ) | , [ , ], ( , ) .

V a b t y

y t t y y t t y t a b t y V

0 0

0 0

Let the maximal interval of the solution ( , , )

to the Cauchy problem ( , ), ( )

be ( , ),

y t t y

y f t y y t y

then for any , : , a b a b

Page 79: Chapter 2 Theory of First Order Differential Equations

0 0( , )t y

Page 80: Chapter 2 Theory of First Order Differential Equations

1 1 0 0( , ( , , ))P t y t t y0 0 1 1 0 0( , , ) ( , , ( , , ))y t t y y t t y t t y

0 0( , )t y

0ta b

VK

1t

1y P

0y

1 1( , )t y

t

( )1 0 0 0 0 1 0 0[| - | | ( , , ) - ( , , ) |]L b ae y y y t t y y t t y

1| - |1 1 0 0 1 1 0 0| ( , , ) - ( , , ) | | - ( , , ) |L t ty t t y y t t y e y y t t y

0 0 0 0( , , )y y t t y

Page 81: Chapter 2 Theory of First Order Differential Equations

Proof:

max 0 0

0

We choose a closed interval [ , ] ( , ) such

that [ , ].

a b I t y

t a b

0 0

We choose small enough such that the stripregion

of ( , , )K y t t y

0 0 {( , ) : [ , ], | ( , , ) | },K t y t a b y y t t y

is contained in the open set U.

By Lemma 3.1, f(t, y) satisfies a Lipschitz condition on K with a Lipschitz constant L.

Page 82: Chapter 2 Theory of First Order Differential Equations

implies- ( - )

1 1 1 0 1 0Set {( , ) : | | , | | / 2} .L b aV t y t t y y e

0 0Then ( , ) .t y V K U

1 1If ( , ) we havet y V1 1 0 0 1 1 1 1 0 0| ( , , ) - ( , , ) | | ( , , ) - ( , , ( , , )) |y t t y y t t y y t t y y t t y t t y

1 11 1 1 1 0 0 1 1 0 0| ( , ( , , )) -[ ( , , ) ( , ( , , ( , , )) ] |

t t

t ty f s y s t y ds y t t y f s y s t y t t y ds

11 1 0 0 1 1 1 1 0 0| - ( , , ) | | ( , , ) - ( , , ( , , )) |

t

ty y t t y L y s t y y s t y t t y ds

From Gronwall inequality we conclude that1| - |

1 1 0 0 1 1 0 0| ( , , ) - ( , , ) | | - ( , , ) |L t ty t t y y t t y e y y t t y

and this concludes the proof.

11 1 0 0 1 1 0 0| - ( , , ) | | ( , , ) - ( , , ) |

t

ty y t t y L y s t y y s t y ds

Since 0 0( , , )y t t y is continuous at 0 ,t t 00,s.t. | - |t t ( )

0 0 0 0 0| ( , , ) - ( , , ) | / 2. L b ay t t y y t t y e

( )1 0 0 0 0 1 0 0 [ | | | ( , , ) ( , , ) |]L b ae y y y t t y y t t y

Page 83: Chapter 2 Theory of First Order Differential Equations

Let : ( an open set of ) be continuous

and satisfy a local Lipschitz condition with respect to .

f U R U R R

y

Corollary

0 0(ii) ( , , ) is a continuous function on .y t t y G

0 0

0 0 0 0

0 0 0 0

For each ( , ) , let the maximal interval of the

solution ( , , ) to the IVP ( , ), ( )

be ( ( , ), ( , )).

t y U

y t t y y f t y y t y

t y t y

0 0 0 0 0 0Then (i) G: ( , ) ( , ), ( , ) is a region;t y t t y t y U

Page 84: Chapter 2 Theory of First Order Differential Equations

0 0( , )P t y

a

b

0 0( , )t y

0 0( , )t y

U

t

0t

0yO

G

0 0( , , )Q t t y

Page 85: Chapter 2 Theory of First Order Differential Equations

Proof:

0 0 0 0 0 0 0 0( , , ) , i.e., ( , ) ( , ), ( , )t t y G t y t t y t y U

Choose a,b, such that

0 0 0 0( , ) ( , )t y a t b t y

From Theorem 3.1, 1 1( , , ) is defined on ,y t t y a t b

(i)

It follows that 0 0( , , )t t y is an interior point of G.This means that G is an open set.

1 1 0 0whenever ( , ) sufficiently close to ( , ).t y t y

From the connectivity of U, it is easy to see G is a connected set, and so G is a region.

Page 86: Chapter 2 Theory of First Order Differential Equations

0 0 2

0 0 0 0 2

Again ( , , ) is continuous at , so 0, . .

| ( , , ) ( , , ) | ,whenever | | .2

y t t y t s t

y t t y y t t y t t

(ii) From Theorem 3.1, we have that

1 1 1 0 00, 0, . . | ( , , ) ( , , ) | .2

s t y t t y y t t y

1 1 0 0

1 1 0 0 0 0 0 0

1 0 1 0

| ( , , ) ( , , ) |

| ( , , ) ( , , ) | | ( , , ) ( , , ) |

, whenever | | ,| | ,| | .

y t t y y t t y

y t t y y t t y y t t y y t t y

t t t t y y

Setting 1 2min{ , }, we have

The proof is complete.

Page 87: Chapter 2 Theory of First Order Differential Equations

2. Continuous Dependence On Parameters

Consider the IVP

0 0( , , ), ( ) ,dy

f t y y t ydt

where is parameter, ( , , ) ( , ),

an open set of .

t y G U

U R R

Page 88: Chapter 2 Theory of First Order Differential Equations

0 0

0 0

Let : ( an open set of )

be continuous and satisfy a local Lipschitz condition

with respect to . For each ( , , ) , let the

maximal interval of the soluti

Theor

on

em:

( , , , ) to

f G R U R R

y t y G

y t t y

0 0 0 0 0 0

0 0

0 0 0 0 0 0

the

IVP ( , , ), ( ) is ( ( , , ), ( , , )).

Then ( , , , ) is a continuous function on

: ( , , ) ( , , ), ( , , ) .

y f t y y t y t y t y

y t t y

t y t t y t y G

Page 89: Chapter 2 Theory of First Order Differential Equations

0 0(2) Smooth dependence with respect to , and .t t y

0 0

We turn next to the question whether supplementary

conditions on ( , ) such as differentiability do imply

that the solution ( , , ) is differentiable.

f t y

y t t y

0We considerfirst the differentiability with respect to .x

In order to obtain an idea of the form of the derivative0 0

0

( , , )y t t y

y

Page 90: Chapter 2 Theory of First Order Differential Equations

we write the Cauchy problem as

0and differentiate formally with respect to .y

0 Exchanging the derivatives with respect to and

we find

t y

0

0 0 0

0

0 0 0

( , , )( , ( , , )), ( , , )

y t t yf t y t t y y t t y y

t

0 0 0

0 0

0

0

0 0 0

0 0

( , , ) ( , ( , , )) ( , , )

( , , )1

y t t y f t y t t y y t t y

t y y y

y t t y

y

Page 91: Chapter 2 Theory of First Order Differential Equations

This formal calculation shows that the function0 0

0

( , , )y t t y

y

is a solution of the linear equation

0 0

This equation is called the variational equation for

the Cauchy problem ( , ), ( ) . y f t y y t y

All the following proof does is to justify this procedure.

00

0

( , ( , , )), ( ) 1

f t y t t yz z z t

y

Page 92: Chapter 2 Theory of First Order Differential Equations

0 0

Let : ( an open set of ) be continuous

and satisfy a local Lipschitz condition. Assume that

( , ) exists and is continuous on . Then the solution

( , , ) of the Cauchy problem

f U R R U R R

f t yU

y

y t t y y

0 0

0 0

( , ), ( )

is continuously differentiable with respect to , , .

f t y y t y

t t y

Theorem 3.2

Page 93: Chapter 2 Theory of First Order Differential Equations

Proof: Let

0 0 0 0

0 0 0 0

( , , ) and ( , , ) (| | ,

is small enough) be the solutions to the Cauchy problem

( , ), ( ) and ( , ), ( ) ,

respectively.

y t t y y t t y

y f t y y t y y f t y y t y

0 0 0 0The integral equations for ( , , ), ( , , ) arey t t y y t t y

00

0 0 0 0( , , ) ( , ( , , )) ,t

ty t t y y f s y s t y ds

00

0 0 0 0( , , ) ( , ( , , )) .t

ty t t y y f s y s t y ds

Page 94: Chapter 2 Theory of First Order Differential Equations

0

( , ( ))( )t

t

f s dsy

Using the theorem of the mean, we have

where 0 1. Note that the continuity of , and ,

f

y

we have

1

( , ( )) ( , ),

f s f sr

y y

1 1where 0 as 0, and 0 0.r r as Thus, for 0, we have

0

( )1 ( , ( ))

t

t

f s dsy

This shows that is the solution of the IVP

1 0 0

( , )[ ] , ( ) 1 .

dz f tr z z t z

dt y

Page 95: Chapter 2 Theory of First Order Differential Equations

This shows that

is the solution

1 0 0

( , )[ ] , ( ) 1 .

dz f tr z z t z

dt y

From the theorem of continuous dependence, we get

is a continuous function of 0 0, , , ,t t z so the limit

0 0

00

( , , )lim

y t t y

y

exists, 0 0

0

( , , )y t t y

y

is the solution of the IVP

0

( , )[ ] , ( ) 1.

dz f tz z t

dt y

and

of the IVP

Clearly, it is a continuous function of

Hence

0

0 00 0

0

( , , )exp{ ( , ( , , ) }.

t

t

y t t yf s y s t y ds

y y

0 0, , .t t y

Page 96: Chapter 2 Theory of First Order Differential Equations

In the same manner, we can prove that 0 0

0

( , , )y t t y

t

Clearly, it is continuous function of

exists and is the solution of the IVP

0 0 0

( , )[ ] , ( ) ( , ).

dz f tz z t f t y

dt y

0 0, , .t t y

Hence

0

0 00 0 0 0

0

( , , )- ( , )exp{ ( , ( , , ) }.

t

t

y t t yf t y f s y s t y ds

y y

Page 97: Chapter 2 Theory of First Order Differential Equations

0 0

0 0

Noting that ( , , ) is the solutionof the Cauchy problem

( , ), ( ) ,

y t t x

y f t y y t y

is continuous function of 0 0, , .t t y

0 0( , , )it follows that

y t t y

t

Page 98: Chapter 2 Theory of First Order Differential Equations

Exercise 3.3

1. Proof:

0 0 0 0

0 0

Since is continuous and satisfy a local Lipschitz condition

on , so ( , ) , the solution ( , , ) to the

Cauchy problem ( , ), ( )

exists, and is unique and continuous depend

f

G x y G y x x y

y f x y y x y

0 0ence on , .x y

Note that ( ,0) 0, so 0 is the solution to ( , ).f x y y f t y

Page 99: Chapter 2 Theory of First Order Differential Equations

x

y

O0x 0x

0y0y

Page 100: Chapter 2 Theory of First Order Differential Equations

(1) (2)

1 0 1

0 0 0

0, 0, | |

| ( , , ) | ,

such that y implies that

y x x y for all x x

Assume that

0 00 0 000 , ( , , ).and x x set y y x x y

0 0

0 0

Since the solution to y = f(x, y),y(x )

is continuous dependence on x ,y ,

y

Page 101: Chapter 2 Theory of First Order Differential Equations

1 2 20

0 0 0 10 0

00

0, 0, | |

| ( , , ) ( , ,0) | | ( , , ) |

.

so for the such that y implies that

y x x y y x x y x x y

for all x x x

00 0 10, | ( , , ) | | | .In particularly y x x y y

Hence, 0 0 0| ( , , ) | ,y x x y whenever x x

Thus 00 0 0| ( , , ) | .y x x y whenever x x x

Page 102: Chapter 2 Theory of First Order Differential Equations

(2) (1) Assume that

2 20

00 0

0, 0, | |

| ( , , ) | .

such that y implies that

y x x y for all x x

0 0

0 0

Since the solution to y = f(x, y),y(x )

is continuous dependence on x ,y ,

y

1 0 2

0 0 0 0 0 1

00

0, 0, | |

| ( , , ) ( , ,0) | | ( , , ) |

.

so such that y implies that

y x x y y x x y x x y

for all x x x

Page 103: Chapter 2 Theory of First Order Differential Equations

1 0 1

0 0 0

0, 0, | |

| ( , , ) | ,

such that y implies that

y x x y for all x x

Note that the solution to 0 0 ( , ), ( ) y f t y y t y

is unique, so

x

y

O0x 0x

0y0y

Page 104: Chapter 2 Theory of First Order Differential Equations

Exercise 3.1

4. 1, are continuous in 0,

2yf f y

So conditions of the existence theorem are satisfied.

It is easy to see that 0y is a solution to the

equation passing through (0,0).

Solving for 1 3

3 23

, we have | | ( ) .2

dyy y x c

dx

Page 105: Chapter 2 Theory of First Order Differential Equations

So all solutions passing through (0,0) are

3

2

0,| | , ( 0).

( ) ,

x cy c

x c x c

Page 106: Chapter 2 Theory of First Order Differential Equations

5.

Proposition 1: y=y(x) is the solution to the initial value problem

0 0( ) ( ), ( )dy

P x y Q x y x ydx

is equivalent to y=y(x) is a continuous solution to the integral equation

00 [ ( ) ( )] .

x

xy y P s y Q s ds

(1)

(2)

Page 107: Chapter 2 Theory of First Order Differential Equations

(ii) Set up a sequence of Picard iterates

(iii)

0

0 0

0 1

( ) ,

( ) [ ( ) ( ) ( )] , 1,2, .x

n nx

y x y

y x y P s y s Q s ds n

( ) [ , ] .ny x is well defined and continuous on

( )ny x ( ), [ , ].y x x

0[ , ] [ , ]

max | ( ) ( ) |, max | ( ) | .x x

Set M P x y Q x L P x

Then1

1| ( ) ( ) | ( ) .( 1)!

nn

n n

MLy x y x

n

Page 108: Chapter 2 Theory of First Order Differential Equations

(iv) y(x) is a continuous solution to the integral equation.

(v) uniqueness.

[ , ]max | ( ) ( ) ( ) | .x

M P x z x Q x

Page 109: Chapter 2 Theory of First Order Differential Equations

6. Proof: Set

Then

and

Therefore

or, equivalently,

( ) ( ) ( ) .t

G t K f s g s ds

( ) ( ), [ , ]f t G t t

( ) ( ) ( ).G t f t g t

( ) ( ) ( ) ( ) ( )( ), [ , ]

( ) ( ) ( )

G t f t g t g t G tg t t

G t G t G t

Page 110: Chapter 2 Theory of First Order Differential Equations

or

or

which implies that

ln ( ) ( ), [ , ]d

G t g t tdt

ln ( ) ln ( ) ( ) , [ , ]t

G t G g s ds t

( ) ( )( ) ( ) , [ , ]

t tg s ds g s ds

G t G e Ke t

( )( ) , [ , ].

tg s ds

g t Ke t

Page 111: Chapter 2 Theory of First Order Differential Equations

Let y(t) and z(t) are both solutions to the given IVP, then

0

0

| ( ) ( ) | | [ ( , ( )) ( , ( ))] |

| ( ) ( ) | .

t

t

t

t

y t z t f s y s f s z s ds

L y s z s ds

From Gronwall inequality, we get

00 0 0| ( ) ( ) | | ( ) ( ) | 0, .

t

tLds

y t z t y t z t e t t

Page 112: Chapter 2 Theory of First Order Differential Equations

0 ,If t t then

0

0 0

| ( ) ( ) | | [ ( , ( )) ( , ( ))] |

| | ( ) ( ) | | | ( ) ( ) | .

t

t

t t

t t

y t z t f s y s f s z s ds

L y s z s ds L y s z s ds

so

00 0 0| ( ) ( ) | | ( ) ( ) | 0, .

t

tL ds

y t z t y t z t e t t

Page 113: Chapter 2 Theory of First Order Differential Equations

7. Assume that the contrary, then there exist two different solutions

1 2 1 2 0 1

1 1 2 1

( ), ( ) ( ) ( ),

( ) ( ).

y x y x with x x x x x

and x x

1 2 0 1( ) ( ) ( ), ( ) 0, ( ) 0,set y x x x then y x y x

This is contrary to

1 2 0 1( , ( )) ( , ( )) 0, .dy

f x x f x x x x xdx

Page 114: Chapter 2 Theory of First Order Differential Equations

9. (1) For any fixed 0 1, ( ), 0,1,2,n nx set x f x n

(2)1 1

1 1 0| | | | 1.n nn nx x N x x N M for all n

We show inductively that

2 1 1 0 1 0| | | ( ) ( ) | | | .x x f x f x N x x NM

Observe first that (1) is obviously true for n=1, since

Next, we must show that (1) is true for n=k+1 if it is true for n=k.

(1)

But this follows immediately, for

Page 115: Chapter 2 Theory of First Order Differential Equations

21| | ,k

k kx x N M

then1

1 1 1| | | ( ) ( ) | | | .kk k k k k kx x f x f x N x x N M

10 1, nSince N so N M (3)

1 12

, ( )n nn

Hence x x x

This implies that { } .nx converges

Page 116: Chapter 2 Theory of First Order Differential Equations

(5) Let * *( )x f x and ( ),x f x

then* * *| | | ( ) ( ) | | |x x f x f x N x x

implies * ,x x since N<1.

* *1

* *

| ( ) ( ) | | | ( ),

( ).

n n n nFrom f x f x N x x and x f x

we have x f x

(4)

Page 117: Chapter 2 Theory of First Order Differential Equations

10. (i) Define the successive approximations

0( ) ( ),x f x and

1( ) ( ) ( , ) ( ) , 1.b

n nax f x K x d n

By induction on n, we can show that ( )n x

is well defined and continuous on [a,b], since

( ) [ , ] ( , ) ([ , ] [ , ]).f x C a b and K x C a b a b

Page 118: Chapter 2 Theory of First Order Differential Equations

Clearly, the sequence

[ , ].a b

(ii) We now show that our successive approximations converges uniformly for t on the interval

This is accomplished by writing ( )n xin the form

0 1 0 1( ) ( ) [ ( ) ( )] [ ( ) ( )]n n nx x x x x x

( )n x converges

if, and only if, the infinite series

1 0 1[ ( ) ( )] [ ( ) ( )]n nx x x x

converges .

Page 119: Chapter 2 Theory of First Order Differential Equations

Set [ , ] [ , ]

[ , ]

max , max ,x a b x a b

a b

M f x L K x

Then 1 0 0,b

ax x K x d , ( )

b

aK x f d ML b a

2 1 1 0,b

ax x K x d 2 2 2

1 0, ( )b

aK x d ML b a

Thus, in turn, implies that

Page 120: Chapter 2 Theory of First Order Differential Equations

Proceeding inductively, we have that

n 1 ( ) [ , ].n n n

nx x ML b a for x a b

Consequently,

converges uniformly

( )n x

on the interval [ , ],a b

if 1

,L b a

then

lim ( ) ( ), ( ) [ , ].nset x x then x is continuous on a b

Page 121: Chapter 2 Theory of First Order Differential Equations

( , ) ( )nK x x converges uniformly

since

| ( , ) ( ) ( , ) ( ) | | ( ) ( ) |n nK x x K x x L x x

and ( )n x

[ , ],a bon

[ , ].a b

(iii) Note that

to

converges uniformly to

Then one can exchange integral and the limit.

( , ) ( )K x x

( )x on

Page 122: Chapter 2 Theory of First Order Differential Equations

Thus

lim ( , ) ( ) ( , ) ( ) ,b b

na anK x d K x d

and ( ) ( ) ( , ) ( ) .b

ax f x K x d

(iV) If ( ) ( ) ( , ) ( ) ([ , ]).b

ax f x K x d C a b

then

0| ( ) ( ) | | ( , ) ( ) |b

ax x K x d

| | ( ).L N b a

where [ , ]

max .x a b

N x

Page 123: Chapter 2 Theory of First Order Differential Equations

Hence, ( ) ( ), [ , ].x x x a b

1 0| ( ) ( ) | | ( , )( ( ) ( )) |b

ax x K x d 2 2 2| | ( ) .L N b a

Proceeding inductively, we have that1 1 1| ( ) ( ) | | | ( )n n n

nx x L N b a

which implies that converges uniformly1

[ , ], | | .( )

a b whenL b a

( )n xon the interval

Page 124: Chapter 2 Theory of First Order Differential Equations

Theorem 1.1 (Existence and uniqueness for the Cauchy problem)

and suppose that

0 0{( , ) :| | ,| | }A t y t t a y y b

:f A R• is continuous,

Then the Cauchy problem

0 0( , ), ( )dy

f t y y t ydt (1)

has a unique solution on0 0[ , ],t h t h

Let

where

( , )min( , ) with max | ( , ) | .

t y A

bh a M f t y

M

• satisfies a Lipschitz condition with respect to y.

Page 125: Chapter 2 Theory of First Order Differential Equations

Proof of the TheoremWe will prove the theorem in five steps:

(i) Show that the initial value problem

0 0( , ), ( )dy

f t y y t ydt

is equivalent to the integral equation

00( ) ( , ( )) .

t

ty t y f s y s ds

(1)

(2)

Specifically, y(t) is a solution of (1) if, and only if, it is a continuous solution of (2).

Page 126: Chapter 2 Theory of First Order Differential Equations

(ii) Construction of the approximating sequence

0

0 0

0 1 0

( ) ,

( ) ( , ( )) ,| | , 1.t

n nt

y t y

y t y f s y s ds t t h n

(iii) Show that the sequence of Picard iteration

converges uniformly on the interval

{ ( )}ny t

0 0[ , ];t h t h

and show that are well defined for all ( )ny t 0;n

and only if, the infinite series

1 0 1[ ( ) ( )] [ ( ) ( )]n ny t y t y t y t

{ ( )}ny t converges if,

converges .

Page 127: Chapter 2 Theory of First Order Differential Equations

(iv) Show that the limit of the sequence { ( )}ny t

is a continuous solution to the integral equation (2).

(v) Show that this solution is unique.