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THEORY OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary Center for Applied Mathematics Virginia Polytechnic Institute and State University Blacksburg, Virginia 24061-0531 MATH 5245 FALL 2012

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Page 1: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

THEORY OF ORDINARYDIFFERENTIAL EQUATIONS

Review of Advance Calculus Topics

John A. Burns

Center for Optimal Design And Control

Interdisciplinary Center for Applied MathematicsVirginia Polytechnic Institute and State University

Blacksburg, Virginia 24061-0531

MATH 5245FALL 2012

Page 2: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

TopicsReview of Differentiation for Vector Valued Functions Partial and Directional Derivatives Derivatives (Fréchet) Gradients, Jacobians and Hessians

Matrix Theory

Page 3: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Calculus for F: D(F) Rn ---> Rm

We review calculus for vector-valued functions of n variables. We then go to the infinite dimensional case. The following references are good …

Robert G. Bartle, The Elements of Real Analysis, John Wiley & Sons, New York, 1976L. V. Kantorovich and G. P. Akilov, Functional Analysis in Normed Spaces, Pergamon Press, New York, 1964.M. Z. Nashed, Differentiability and Related Properties of Nonlinear Operators: Some Aspects of the Role of Differentials in Nonlinear Functional Analysis, in Nonlinear Functional Analysis and Applications, Academic Press, New York, 1971.J. M. Ortega and W. C. Rheinboldt, Iterative Solution of Nonlinear Equations in Several Variables, Academic Press, New York, 1970.A. E. Taylor, An Introduction to Functional Analysis, John Wiley & Sons, New York, 1967.E. Zeidler, Applied Functional Analysis, Springer-Verlag, New York, 1995.

Page 4: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Finite Dimensional Spaces1

2

.:

.

.

i

n

xx

x R

x

1

2

.:

.

.

i

n

xx

x C

x

COLUMN VECTORS

iNi

n

i

pip

n

ii

n

ii

nTn

xx

pxx

xx

xxx

Rxxxx

p

max

1 ,

,...,,

1

1

11

1

2

2

21

1

NORMS (SAME for Complex Spaces)

c of moduluscomplex

of valueabsolute22

babiac

rr

and

i) 0 and 0 if and only if 0

ii) x , (or )

iii) , for , (or )

n n

n n

R

x x x

x x R C

x y x y x y R C

A Norm on is a functionsatisfying

RRn :nR

R = Real Numbers R+ = [0, +)C = Complex NumbersRn = n-dimensional Euclidean Space = Cn = n-dimensional Complex SpacexT = [x1, x2, …,xn]

- inequality

Page 5: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Finite Dimensional SpacesThe vector space Rn with a norm || || is a normed linear space. Inparticular, the pair (Rn , || ||2) is called n-dimensional Euclidean space.

2: 12

1

nx x xii

1: | | 11

nx x xii

x1

x2

The distance between two vectors x and y in Rn is given by dist(x,y) = ||x - y||.

The geometry and differentiability of different norms are DIFFERENT!

Page 6: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Finite Dimensional SpacesEquivalent Norm Theorem:

If ( , ) is one of the finite dimensional normed linear spaces ( , ) or

( , ), then there are constants 0 and 0 such that for any 1

nX R nC m M p

. m x x M xp p

2 1 2x x n x

2x x n x

1x x n x

EXAMPLES

Page 7: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Finite Dimensional Spaces

ˆ ˆ( , ) :B x x X x x

Open Ball About A Point Closed Ball About A Point

ˆ ˆ( , ) :B x x X x x

For k = 1,2,3, … let be a sequence of vectors in

Rn. We say that {xh} converges to x in Rn if

and we write

1 2[ .. ]k k k k Tnx x x x

lim 0,k

k x x

k kx x

For each > 0 there is a K() > 1 such that if k ≥ K(), then

.kx x

Page 8: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Finite Dimensional Spaces

NOTE: Because of the Equivalent Norm Theorem if || ||p is any norm on Rn, then

2lim - 0k

k x x

lim - 0k

pk x x

if and only if

NOTE:

IMPLIES that for i= 1, 2 , …, n

k

kx x

ki ikx x

AND :

for all i= 1, 2 , …, n IMPLIES

k

i ikx x

k

kx x

Page 9: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Inner ProductsAn inner product on Rn is a mapping such that , : n nR R R

n

n

n

Rzyx

Ryx

Ryx

x

R

,, ,yz,yx, yz,x iv)

,for xy, yx, iii)

, ,yx, yx, ii)

0 ifonly and if 0xx, and 0xx, i)

and

EXAMPLE: )(... ,1

xyyxyxyx Tn

iii

An inner product on Cn is a mapping such that CCC nn :,

n

n

n

Czyx

Cyx

Cyx

x

C

,, ,yz,yx, yz,x iv)

,for xy, yx, iii)

, ,yx, yx, ii)

0 ifonly and if 0xx, and 0xx, real, is xx, i)

_____

and

EXAMPLE: )*(... ,1

xyxyyxyxyx Tn

iii

Page 10: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Inner Product Spaces

______ _________ ______

__________ ________________

andFor all , ,

, and

x,y z y z,x y,x z,x x,y x,z

nC

α y y αy

x y z C

x, y ,x ,x ,x x, y

NOTE:

A norm || || and an inner product <· , · > are compatible if x,xxx,xx 2or

n

ii

n

iii xxxxxx

1

2

12

||,EXAMPLE:

REMARK: If p 2 then there is NO inner product <· , · > with x,xxp

If <· , · > is an inner product on Rn , then the pair (Rn , <· , · > ) is called aninner product space. Same for (Cn , <· , · > ).

Page 11: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Results for Inner Products

Schwarz Inequality: yxy,x

Parallelogram Law: 2222 2 yxyxyx

Two vectors are call orthogonal if )(or , nn CRyx 0.x,y

Pythagorean Theorem: .yxyx,y,x 222 then0 If

x

y

x

y

x y

Page 12: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Matrix Notation

nm

m,nm,m,

,n,,

,n,,

i,j R

a..aa

aaaa..aa

a

::::

..

21

22212

12111

A

We use standard matrix notation ... for real matrices

mn

m,n,n,n

m,,,

m,,,

T

i,jT R

a..aa

aaaa..aa

a

::::

..

21

22221

11211

A

nni,jn R

..

..

100::::0..10001

II

AND standard terms ... diagonal tridiagonal upper triangular :

Symmetric

skew-symmetric

positive definite

orthogonal

AA T

AA T

nT Rxxx 0 ,0AIAA T

Page 13: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Matrix Notation

11 1 2 1

2 1 2 2 2

1 2

..

: : : :

, , ,n

, , ,n m ni, j

m, m, m,n

a a .. aa a a

a C

a a .. a

A

We use standard matrix notation ... for complex matrices

11 2 1 1

1 2 2 2 2

1 2

..

: : : :

, , m,

T, , m,T n m

i, j

,n ,n m,n

a a .. aa a a

a C

a a .. a

A

nni,jn R

..

..

100::::0..10001

II

AND standard terms ...

diagonal tridiagonal upper triangular :

self-adjoint (Hermitian)

skew-adjoint

positive definite

unitary

* A A* A A

* 0, 0 nx x x C A* A A I

11 2 1 1

1 2 2 2 2*

1 2

..

: : : :

, , m,

T, , m, n m

i, j

,n ,n m,n

a a .. aa a a

a C

a a .. a

A

Page 14: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Matrix Notation

MATRIX NORMS ...

11 1 2 1

2 1 2 2 2

1 2

..

: : : :

, , ,n

, , ,n m ni, j

m, m, m,n

a a .. aa a a

a R

a a .. a

A

2/1

1 1

2

,

m

i

n

jjiF aAFROBENIUS NORM ...

p

p

xp x

xAA sup

0P - NORM ...

FACTS

22 n AAA F max max ,2, nm jiji aa A

AAA12

m

ijia

1,j1 ||max A

n

jjia

1,i

||max A

Page 15: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Matrix Notation

nm

m,nm,m,

,n,,

,n,,

i,j R

a..aa

aaaa..aa

a

::::

..

21

22212

12111

A sn

n,sn,n,

,s,,

,s,,

i,j R

b..bb:.::

bbbb..bb

b

21

22212

12111

B

FFF BABA

THESE MATRIX NORMS ARE MUTUALLY CONSISTENT ...

ppp BABA

IF Q AND Z ARE BOTH ORTHOGONAL, THEN

FF AZAQ 22 AZAQ

Gene H. Golub and Charles Van Loan, Matrix Computation, third edition, The Johns Hopkins University Press, London, 1996.

Page 16: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Functions of n VariablesLet D(F) Rn be a subset of Rn and let F: D(F) --->Rm be a function with domainD(F) Rn and range R(F) in Rm.

One of the most fundamental problems in engineering and science is: Given y Rm, find x D(F) Rn such that

F(x) = y (1)

EXISTENCE: If F is onto Rm (i.e., if R(F) = Rm) then there exists at least onesolution to (1).

UNIQUENESS: If F is one-to-one (i.e, F(x1) = F(x2) implies that x1= x2), then thesolution to (1) is unique.

MOST IMPORTANT PROBLEMS

ACTUALLY COMPUTING THE SOLUTION

FIND CHECKABLE CONDITIONS FOR EXISTENCE & UNIQUENESS

DEVELOP FAST & ACCURATE ALGORITHMS - SOFTWARE TOOLS

Page 17: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Functions of n Variables

The function F is locally one-to-one at the point x D(F) Rn, if there is a > 0 such that F restricted to the set D(F)B(x, ) is one-to-one.

The function F is one-to-one on the set D(F) Rn, if F restricted to the setD(F) is one-to-one.

If F is one-to-one on the set D(F) Rn, then there exists a function F -1 from = F( ) Rm into Rn such that

F(F -1(y)) = y for all y AND F -1(F(x)) = x for all x

The function A: D(A) ---> Rm is linear ifn i) ( ) is a linear subspace of D RA

1 2 1 2 1 2ii) If and , ( ), then , R x x D A ( x + x )= (x )+ (x ) A A A

AND

A linear function : Rn ---> R is called a linear functional.

Page 18: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Functions of n VariablesLet F: D(F) Rn --->Rm and G: D(G) Rm --->Rk be functions. Thecomposite function is the function G o F :D(GoF) Rn --->Rk is definedon the domain

( ) ( ) : ( ) ( ) ( ) nD G F x D F F x D G D F R

by [G o F ](x) = G(F(x))

F G

G o F

xRn F(x)Rm

G(F(x))

Rk

Page 19: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

CalculusIf F: D(F) Rn ---> Rm is a function with domain D(F) Rn and range R(F) in Rm,then F is continuous at p Rn, ifi) p D(F)ii) For each > 0, there is a = (p, ) > 0, such that if x D(F) B(p, ),

then || F(x) - F(p) ||Rm <

We say that F is continuous, if F is continuous at each x D(F)

NOTE: i) and ii) are equivalent to ... - 0lim ( ) - ( ) 0m

nRRx p

F x F p

The function F: D(F)Rn ---> Rm is a contraction if there is a < 1 such that ifx0 , x1 D(F) , then || F(x1) - F(x0) ||Rm || x1 - x0 ||Rn

Page 20: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Abuse of NotationLet D(F) Rn be a subset of Rn and let F: D(F)Rn --->Rm be a functionwith domain D(F) in Rn and range R(F) in Rm.

1

21

11 1

22 2 1

1

2

( ):

( )( ) ( )

( ) :

( )

( ):

n

nn m

m

n

xx

F

x

xx F x

xx F x F

F(x) Fx

x F x

xx

F

x

Tn

n

xxx

x

xx

x ..: 12

1

1 1 1 2

2 2 1 21 2

1 2

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

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

n

nn

m m n

F x F x x xF x F x x x

F(x) F x x x

F x F x x x

Page 21: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Notation

If A: D(A)Rn ---> Rm is a linear function with domain, then one can show that A is continuous. Moreover, A is bounded. In particular, there is a M 0 such that for all x D(A) one has

|| A(x) ||Rm M || x ||Rn.

The operator norm on A is defined to be

0

( )sup m

n

R

x R

A xA A

x

RECALL: All linear operators from Rn to Rm have a matrix representation.Actually, if one selects basis for Rn and Rm, then there exist a mn matrix

such that

11 1 2 1

2 1 2 2 2

1 2

..

: : : :

, , ,n

, , ,n m ni, j

m, m, m,n

a a .. aa a a

a R

a a .. a

A

( )A x x A( )A x x AOPERATOR MATRIX

Page 22: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Matrix Representations

The standard unit vectors ei = [0 0 … 0 1 0 … 0]T

ith position

x=[x1,x2]T

x=[x2,-x1]T

0( ) rotate clockwise by 90A x

1

2

0 1( )

1 0x

x xAx

A

WARNING: The use of matrices as representations of linear operators is important. However, be sure not to confusethe representation (MATRIX) with the operator A.A

Page 23: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Partial DerivativesLet F: D(F) Rn ---> R1 be a real-valued function of n variables.The partial derivative xiF(p) at p is a number Di=Di (p) satisfying:For each > 0, there is a = (p, ) > 0, such thatfor each t with - < t < , [p + tei] D(F) and

| F(p + tei) - F(p) - Di t | | t | (2)or equivalently,

| F(p1, p2, …,pi + t, …pn) - F(p1, p2, …,pi, …pn ) - Di t | | t |. (3)

1t 0lim | [ ( ) ( )] | 0i

it F p te F p D

NOTE: The partial derivatives will be denoted by several symbols ...

APPLYING THE CHAIN RULE (IF POSSIBLE)

0( ) ( ) ( )

i

ididt x x pt

F p te F p x F x

Page 24: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Partial Derivatives

i i i

F(p)i ix x x x p

D F(p) x F(p) F(x)

IMPORTANT REMARK: The partial derivative of a real-valued function F at a point p is a NUMBER!

HIGHER ORDER PARTIAL DERIVATIVES ...2

22

iixx x p

F(p) F(x)

NEED GENERAL NOTATION: Let s=(s1, s2, …, sn) be a multi-index,where each si is a non-negative integer.

1 2

1 2

...

1 2

( ) ( )...

N

N

s s ss

ss sN

D F p F px x x

Let |s| = s1 + s2 + … + sn and define the mixed partial derivative DsF(p) by

(0,0,...,0) 0D F(p) D F(p) F(p)

AGREE THAT

Page 25: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Partial Derivatives

EXAMPLE: In R2 if s=(1,1), then 1 1 2

s (1,1)

1 2 1 2

D ( ) D ( ) ( ) ( )F p F p F p F px x x x

EXAMPLE: In R2 if s=(2,0), then2 0 2

s (2,0)2 0 21 2 1

D ( ) D ( ) ( ) ( )F p F p F p F px x x

EXAMPLE: In R2 if s=(2,0) and r=(0,2), then

2 2(2,0) (0,2)

2 21 2

[ ] ( ) ( ) ( ) ( ) ( ) ( )s rD D F p D F p D F p F p F p F px x

EXAMPLE: In R2 if s=(1,0) and r=(0,1), then

(1,0) (0,1)

1 2

[ ] ( ) ( ) ( ) ( ) ( )s rD D F p D F p D F p F p F px x

Page 26: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Variations and Differentials

There are various notations and terms used for this derivative:

0( ; ) [F( )] ( , )d

dt ttF p p V p

The first variation of F at p in the direction of , The directional derivative of F at p in the direction , (misleading)The Gateaux variation at p in the direction ...

Let Rn be a “direction”. If for each > 0, there is a = (p, ) > 0, such that for each t with - < t < , [p + t ] D(F) and the limit (in R1)

exists, then this limit is called the directional derivative of F at p in thedirection .

10 0

[F( )] lim( )[F( ) ( )]ddt tt t

tp p t F p

If F: D(F) Rn ---> R1, then the partial derivative xiF(p) at p is the first variation of F in the direction of the unit vector ei.

0

1( ) ( ) lim ( )[ ( ) ( )] ( ; )i ii

i t tF p x F p F p te F p F p e

x

Page 27: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Variations and Differentials? WHEN DO THESE VARIATIONS EXIST ?

REQUIRES:

10

For sufficiently small ( )AND lim [ ( ) ( )]

EXISTStt

t p t D F

F p t F p

0( ; ) [F( )]d

dt ttF p p

1

2

( )

( )

:)

( )

(

n

x

x

x

F p

F p

F p

F p

If for all i = 1, 2, …, n the partial derivativesexist, then we can define the gradient vector

i iix x x pF(p) x F(p) F(x)

Page 28: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Variations and DifferentialsIF the CHAIN RULE can be used ...

1 1 2 2 1 1 2 21

( , ,..., ) ( , ,..., )i

nd

N N N N idt xi

F p t p t p t F p t p t p t

At t = 0

1 1 2 2 1 201

( , ,..., ) ( , ,..., ) , ( )i

Nd

N N N idt xti

F p t p t p t F p p p F p

Thus

( ; ) , ( ) [ ( )]TF p F p F p (4)

WARNING: (4) does not always hold!

Page 29: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The Gateaux Derivative

If F(p;) exists for all Rn AND is linear in , then we can define athe Gateaux Derivative.

NOTE: F(p) Rn is a vector. It is not a “derivative”. So,what do we mean by a “derivative”? We start with a weak notion of thederivative and the extend to the stronger notion.

Assume F: D(F) Rn ---> R1 and p int[D(F)]. If the first variation F( p ; )of F at p exists for all Rn AND for 1 , 2 Rn ,

F( p ; 1 + 2 ) = F( p ; 1 ) + F ( p ; 2 ),

(i.e. F( p ; ) is linear in ), then we say that F is Gateaux-differentiableat p. If = p is the (unique) linear functional p: Rn ---> R1 defined byp( ) = F( p ; ), then p is called the Gateaux Derivative of F at p.

The Gateaux Derivative is a linear functional.

Page 30: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Gateaux Derivative

Reisz Representation Theorem. If : Rn ---> R1 is a linear functional onRn,, then

i) is continuous,

and

ii) there exists a fixed vector a Rn (depending on ) such that forall Rn

( ) = < , a > (5)

To make the Gateaux derivative something useful, we need the followingversion of the Reisz Representation Theorem.

If F is Gateaux differentiable at p we can apply the Reisz Representation Theoremto p( ) = F( p ; ), so it follows that there is a unique vectora = a(p) Rn such that for all Rn ,

T

1

( ; ) ) , [ ( )] [ ( )] ( ) .n

p i ii

F p (η a p a p a p

(6)

Page 31: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Gateaux Derivative

IMPORTANT: The linear functional p( ) = f( p ; ) is theGateaux derivative at p. The vector a(p) is just a matrix representation ofthis linear functional.

Note that the linear functional f( p ; )=p: Rn ---> R1 is the Gateaux-derivativeof F at p int[D(F)] if and only if for each Rn

OR EQUIVALENTLY

0lim ( 1/ ) [ ( ) ( )] ( ) 0pt

tt F p F p t

(7)

0

lim (1/ ) [ ( ) ( )] ( ) 0T

ttt F p F p t a p

(8)

Page 32: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Gateaux DerivativeIf F: D(F) Rn ---> R1 is Gateaux-differentiable at p int[D(F)], then the

partial derivatives xiF(p) at p exist. Let a(p) = [a(p)1, a(p)2 , …, a(p)n]T Rn

be the vector defined by (5). It follows that

We have the following theorem.

1

2

( )

( )( ) ( ) .

:( )

n

x

x

x

F p

F pa p F p

F p

(9)

Theorem D1. If F: D(F) Rn ---> R1 is Gateaux differentiable atp int[D(F)], then the gradient of F at p exists, and p( ) = F( p ; ) has the representation

1( ; ) , ( ) ( )

n

i ii

F p F p x F p

(10)

Page 33: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Gateaux DerivativeRECALL ...If A: D(A) Rn ---> Rm is a linear function with domain D(A) Rn and rangeR(A) in Rm, then the operator norm on A is defined to be

n

m

R

R

x x)x(

supA

AA 0

(11)

If f( p ; ) =p : Rn ---> R1 is the Gateaux derivative of F at p, then it is a linearfunctional and the (operator) norm of p is given by

0 0 0

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

n n n

Tp

p pR R R

F p F p

(12)

Page 34: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The DerivativeBUT … what is “the derivative” of a function F: D(F) Rn ---> R1 ? Best tothink of the derivative as a linear function that approximates F locally.

F(x) = (x +1)2 - 1 F( p ; ) = 2(p +1)

Let p denote the linear function with slope F'(p) = 2(p+1). If we look atp = 0, then 0( ) = 2 is a linear approximation to F(·) near p = 0.

-2 -1.5 -1 -0.5 0 0.5 1 1.5 2 2.5 3-4

-2

0

2

4

6

8

10

12

14

16

F()

0( )0( ) = F( 0 ; )

p=0

Page 35: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The Fréchet Derivative

Let F:D(F) Rn ---> R1 be a real-valued function and assumep int[D(F)]. We say that F is (Fréchet) differentiable at p if thereexists a linear functional D :Rn ---> R1 such that for each > 0, thereis a = (p, ) > 0 such that if

0 < || x - p || Rn < ,then

i) x D(F) (13)

ii) | F(x) - F(p) - D(x - p) | || x - p || Rn (14)

If F: D(F) Rn ---> R1 then the (Fréchet) derivative of F at a point p is alinear function D:Rn ---> R1 that “approximates F near p”.

BASIC IDEA …

Notation varies and we shall use ... D = [DF(p)] = DxF(p) = F´(p)

The (Fréchet) Derivative is the LINEAR OPERATOR DxF(p)

Page 36: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The Fréchet DerivativeLet F:D(F) Rn ---> R1 be (Fréchet) differentiable at p with derivativeDxF(p) :Rn ---> R1. Given any > 0, there is a = (p, ) > 0 such that if0 < || x - p || Rn < , then x D(F) and then

| F(x) - F(p) – [DxF(p)](x - p) | || x - p || Rn

Let = x - p. Note that p + = x D(F), 0 < || || Rn < and

| F(p + ) - F(p) - [DxF(p)]() | || || Rn

or equivalently,

(1/ || || Rn) | F(p + ) - F(p) - [DxF(p)]() |

Thus, the linear functional DxF(p) :Rn ---> R1 is the (Fréchet) derivative of thefunction F:D(F) Rn ---> R1 at x = p if and only if

1lim [ ( ) ( )] [ ( )]( ) 0.0 n

xR

F p F p D F p

(15)

Page 37: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The Fréchet DerivativeTheorem D2. If F: D(F) Rn ---> R1 has a Fréchet derivative p int[D(F)], then F has a Gateaux derivative at p and the two derivatives are equal. Inparticular, DxF(p) = p( ) = f( p ; ).

There exist functions F: D(F) Rn ---> R1 such that at p int[D(F)]:

(1) F has a Gateaux differential (first variation) at p but F is not Gateauxdifferentiable at p.

(2) F has a Gateaux derivative at p but F is not Fréchet differentiable at p.

COMMENTS

Problem (P1): Let F :R2 ---> R1 be defined by 2

2 4 ,( , )

0,

x yx y

F x y

(16)(x , y) (0 , 0)

(x , y) = (0 , 0).

Show that F( 0 ; ) exists for all R2 but F does not have a Gateauxderivative at 0 = [0 , 0]T. Also, F is NOT continuous at 0!

Page 38: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The Fréchet Derivative

3

4 2 ,( , )

0,

x yx y

F x y

(17)(x , y) (0 , 0)

(x , y) = (0 , 0)

Problem (P2): Let F :R2 ---> R1 be defined by

Show that F has a Gateaux derivative F( 0 ; ) at p = 0=[0 , 0]T, but F does not have a Fréchet derivative at p = 0=[0 , 0]T.

2

2

( )

2 (2 )

2 ,( , )

0,

x

x

yey eF x y

(18)x 0

x = 0

Problem (P3): Let F :R2 ---> R1 be defined by

Show that F has a Gateaux derivative F( 0 ; ) at p = 0=[0 , 0]T,but F is not continuous at p = 0=[0 , 0]T.

Page 39: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The Fréchet Derivative

,( , )

0,

xy

F x y

(19)y 0

y = 0

Problem (P4): Let F :R2 ---> R1 be defined by

Show that f has partial derivatives at p = 0=[0 , 0]T, but F( 0 ; ) does notexist unless 12 = 0. Also, F is not continuous at (0, 0) = 0.

2 2 ,( , )

0,

x yF x y

(20)if both x and y are rational

otherwise

Problem (P5): Let F :R2 ---> R1 be defined by

Show that F is continuous at only one point p = 0=[0 , 0]T, andyet F is Fréchet differentiable at p = 0=[0 , 0]T.

Page 40: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The Fréchet DerivativeLet D(F) Rn be a subset of Rn and let F: D(F) ---> R1 be a real-valuedfunction of n variables. We say that F is differentiable on the set D(F), if F is Fréchet differentiable at each point x D(F).

Mean Value Theorem For Functionals. Let F: D(F) Rn ---> R1. Assume that F is Fréchet differentiable at all points in theopen set D(F). If x and y are two elements in such that the linesegment {z = x + (1- )y : 0 1 is contained in , then there isa c with 0 < c < 1 such that

F(y) - F(x) = [DxF(c x+(1 - c)y)](y – x) (21)

… OR by defining c = c x+(1 - c)y, we have

F(y) - F(x) = [DxF(c)](y – x) (22)

| F(y) - F(x) | | DxF(c)( y – x) | || DxF(c)|||( y – x) | (23)

IMPLIES

Page 41: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The Mean Value Theorem

c = c x+(1 - c)y

xy

c = c x+(1 - c)yx

y

ASSUMPTIONS SATISFIED ASSUMPTIONS FAIL

Page 42: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The Mean Value Theorem

c = c x+(1 - c)yx

y

If is convex, then the theorem applies to all x and y in .

Let F: D(F) ---> R1 be a real valued function of n variables. If D(F), then we say that F is Holder continuous on the set if there exists constants M 0 and (0, 1] such that for all x, y ,

| F(x) - F(y) | M || x - y||. If = 1, then we say that F is Lipschitz continuous.

Page 43: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Functions F: D(F) Rn ---> Rm

1 1 1 2

2 2 1 21 2

1 2

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

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

n

nn

m m n

F x F x x xF x F x x x

F x F x x x

F x F x x x

If F: D( F ) Rn ---> Rm is a function with domain D( F ) Rn and range R(F )in Rm, then F has the form

where for i = 1, 2, …, m, Fi is a real valued function with domain D( Fi ) Rn

and range R( Fi ) R1.

,i

i j j

F (p)i j i j i ix x x x p

D F (p) x F (p) F (x)

Each function Fi: D(F) ---> R1 fits into the previous framework. For example,the definitions and results involving partial derivatives, Gateaux variations,and Fréchet derivatives hold. The notation is as expected … e.g.

Page 44: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Functions F: D(F) Rn ---> Rm

There are various notations and terms used for this derivative:

0( ; ) [F( )] ( , )d

dt tmt RF p p V p

The first variation of F at p in the direction of , The directional derivative of F at p in the direction , (misleading)The Gateaux variation at p in the direction ...

Let Rn be a “direction”. If for each > 0, there is a = (p, ) > 0, such that for each t with - < t < , [p + t ] D(F) and the limit (in Rm)

exists, then this limit is called the directional derivative of F at p in thedirection .

10 0

[F( )] lim( )[F( ) ( )]ddt tt t

tp p t F p

NOTE: These variations are vectors in the range space Rm

Page 45: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Variations and Differentials? WHEN DO THESE VARIATIONS EXIST ?

REQUIRES:

10

For sufficiently small ( ) AND lim [ ( ) ( )] ( ; )

EXISTStt

m

t p t D FF p t F Rp F p

0( ; ) [F( )]d

dt ttF p p

1

2

( )

( ), 1, 2,...,

:( )

( )

n

ix

ix

ix

i

F p

F pF p

i m

F p

If for all i = 1, 2, …, n the partial derivativesexist, then we can define the gradient vectors

j ji j i ix x x pF (p) x F (p) F (x)

Page 46: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Jacobian Matrix

1

2

1 2

( )

( )[ ] ( ) ( ) ( )

( )

( )n

n

Tix

ixTi i ix x x

ix

i

F p

F pF F F

F

F

p

p

x x x

If for all i = 1, 2, …, n the partial derivativesexist, then we can define the Jacobian matrix

j ji j i ix x x pF (p) x F (p) F (x)

1 2

1 2

1 2

1 1 1

2 2 2

( ) ( ) ( )

( ) ( ) ( )

( ) ( )

( ) ( ) ( )

|

n

n

n

x x x

x x x

m n

m m mx x x

F F F

F F F

F F R

F F F

J J

x p

x p

x x x

x x x

p x

x x xAlso, since

Page 47: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Jacobian Matrix

1 2

1 2

1 2

1 1 1 1

2 2 2 2

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

( )

[ ( )]( ) ( ) ( )

n

n

n

Tx x x

Tx x x

Tmm m mx x x

F p F p F p F pF p F p F p F p

F

F pF p F p F p

J

p

NOTE: JF(p) Rm n is a matrix. It is not a derivative. So, again we have todefine what we mean by a “derivative”? The definitions are the same as for thereal valued functions …

Page 48: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The Gateaux Derivative

If F(p;) exists for all Rn AND is linear in , then we can define athe Gateaux Derivative.

Assume F: D(F) Rn ---> Rm and p int[D(F)]. If the first variation F( p ; )of F at p exists for all Rn AND for 1 , 2 Rn ,

F( p ; 1 + 2 ) = F( p ; 1 ) + F ( p ; 2 ),

(i.e. F( p ; ) is linear in ), then we say that F is Gateaux-differentiableat p. If L = Lp is the (unique) linear function Lp: Rn ---> Rm defined byLp( ) = F( p ; ), then Lp is called the Gateaux Derivative of F at p.

The Gateaux Derivative is a linear operator

: n mpL R R

Page 49: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Gateaux Derivative

Reisz Representation Theorem. If L: Rn ---> Rm is a linear operator onRn,, then

i) L is continuous,

and

ii) there exists a matrix L R m n (depending on L and a basis for Rn and Rm) such that for all Rn

L( ) = L

To make the Gateaux derivative something useful, we need the followingversion of the Reisz Representation Theorem.

If F is Gateaux differentiable at p we can apply the Reisz Representation Theoremto L( ) = F( p ; ), so it follows that there is a matrixL = L(p) R m n such that for all Rn ,

( ; ) ) ( )pF p L (η p L

Page 50: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Gateaux Derivative

IMPORTANT: The linear function Lp( ) = f( p ; ) is the Gateaux derivative of F at p. The matrix L(p) is just a matrix representation of this linear function.

Note that the linear functional f( p ; )= Lp: Rn ---> Rm is the Gateaux derivativeof F at p int[D(F)] if and only if for each Rn

OR EQUIVALENTLY

0lim ( 1/ ) ( 1/ )[ ( ) ( )] ( ) 0mp Rt

tt t F p F p L

0

lim (1/ )[ ( ) ( )] ( ) 0mRttt F p F p p

L

Page 51: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Gateaux DerivativeIf F: D(F) Rn ---> Rm is Gateaux differentiable at p int[D(F)], then the

partial derivatives xjFi(p) at p exist. Select the standard basis for Rn and Rm

and let

Theorem D3. If F: D(F) Rn ---> Rm is Gateaux differentiable atp int[D(F)], then the Jacobian matrix of F at p exists, and Lp( ) = F( p ; ) has the representation

( ; ) [ ( )]F p F p J

1 2

1 2

1 2

1 1 1 1

2 2 2 2

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

( )

[ ( )]( ) ( ) ( )

n

n

n

Tx x x

Tx x x

Tmm m mx x x

F p F p F p F pF p F p F p F p

F

F pF p F p F p

J

p

Page 52: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Gateaux DerivativeRECALL ...

If A: D(A) Rn ---> Rm is a linear function with domain D(A) Rn and rangeR(A) in Rm, then the operator norm on A is defined to be

n

m

R

R

x x)x(

supA

AA 0

If f( p ; ) =Lp : Rn ---> Rm is the Gateaux derivative of F at p, then it is a linearoperator and the (operator) norm of Lp is given by

0 0

( ) [ ( )]sup sup [ ( )]m m

n n

p R Rp p

R R

L F pL L F p

JJ

Page 53: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The Fréchet Derivative

Notation varies and we shall use ... D = [DF(p)] = DxF(p) = F´(p)

The (Fréchet) Derivative is the LINEAR OPERATOR D

Let F:D(F) Rn ---> Rm be a vector-valued function and assumep int[D(F)]. We say that F is (Fréchet) differentiable at p if thereexists a linear operator D :Rn ---> Rm such that for each > 0, thereis a = (p, ) > 0 such that if

then

i) x D(F)

and ii) [ ( ) ( )] ( ) m nR R

F x F p D x p x p

0 nRx p

: n mD R R

Page 54: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

The Fréchet Derivative

If F is Fréchet differentiable at p we can apply the Reisz Representation Theoremto D( ) = [DxF( p )]() to obtain a matrix representation with respect to the standardbasis …

[ ( )]( ) [ ( )]xD F p F p J[ ]( ) [( ) ( )]xD F p F p J

OPERATOR MATRIX

Theorem D4. If F: D(F) Rn ---> Rm is Fréchet differentiable atp int[D(F)], then the Jacobian matrix of F at p exists, F is continuous at p and has the representation

[ ( )]( ) [ ( )]xD F p F p J

Page 55: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Two Theorems

Theorem D5. If F: D(F) Rn ---> Rm and Jacobian matrix of F atp int[D(F)] exists and is continuous in an open ball

about p, then F is Fréchet differentiable at p.

( , ) : nn

RB p x R x p

Mean Value Theorem For Vector Valued Functions. Let F: D(F) ---> Rm.Assume that F is Fréchet differentiable at all points in an open set D(F). If x and y are two elements in such that the linesegment {z = x + (1- )y : 0 1 is contained in , then there isa c with 0 < c < 1 such that for c = c x+(1 - c)y,

CAN NOT SAY … [F(y) - F(x)] = [DxF(c)]( y – x)

( ) ( ) [ ( )]( ) ( )m m nx xR R RF y F x D F y x D F yc c x

Page 56: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Analysis of F: D(F) Rn ---> Rm

In order to use these concepts we need to know when the usual “calculus” results hold. The important results for this topic are:

• Taylor’s Theorem• Chain Rule• Inverse Function Theorem • Implicit Function Theorem• Necessary conditions for optimization• Higher order derivatives• Convexity

We will cover these topics when needed and indicate where proofs can be found in the references.

We present two important results

Page 57: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Chain RuleChain Rule for Fréchet derivative. Let F: D(F) Rn --->Rm andG: D(G) Rm --->Rk be functions. If F has a Fréchet derivativeat p and G has a Fréchet derivative at y = F(p), then the composite functionG o F has Fréchet derivative at p and

for all Rn. Or ….

[ ( )( )]( ) [ ( ( ))] [ ( )]( )x y xD G F p D G F p D F p

( )[( )( )] [ ( ) ] [ ( )]| y F p

d d

dy dx

d G F p G y F pdx

DOES NOT HOLD for Gateaux derivative

[( )( )] [( ( ( ))] [ ( ( ))] [ ( )]x xD G F p D G F p G F p F p

Page 58: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Partial Fréchet Derivatives Let be the product space with norm defined by

If F : D(F) Rn Rp ---> Rm is a function of the two variables x and q, then we can define the partial Gateaux and Fréchet derivatives. If p = ( x0 , q0 )T int[D(F)], then define the domain

D( F1 ) = {x Rn : (x , q0 )T int[D( F)]}

and the function F1 : D( F1 ) Rp ---> Rm by

F1(x) = F( x , q0 ) Rm.

If F1(x) = F( x, q0 ) has a Gateaux (Fréchet) derivative at x = x0 , then we say that F( x, q0 ) has a first partial Gateaux (Fréchet) derivative atz0 = p and we denote this derivative by DxF( x0 , q0 ) or D1F(x0 , q0 ) or xF(x0 , q0 ). Likewise, we can define qF(x0 , q0 ).

n pZ R R

2 2n p

T

R Rx q x q

The partial Fréchet derivatives are LINEAR OPERATORS

Page 59: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Partial Fréchet DerivativesNote that at p = ( x0 , q0 )T int[D( F )], then the partial Fréchet derivative xF(x0 , q0 ) is a continuous linear operator [xF(x0 , q0 )]: Rn ---> Rm and qf(x0 , q0 ) is a continuous linear operator [qF(x0 , q0 )]: Rp ---> Rm.

Assume F: D( F ) Rn Rp ---> Rm is a Fréchet differentiable function of the form

If all the partial derivatives exist and are continuous,

on the open set , then we say that F is smooth on and write

1 1 2 1 21

2 1 2 1 221 2 1 2

1 2 1 2

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

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

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

T

n p

n pn p

m n pm

z x q

F x x x q q qF x qF x x x q q qF x q

F z F x q F x x x q q q

F x x x q q qF x q

( , ) ( , ) and i i

i i

F x q F x qx q

1( )F C

Page 60: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Partial Fréchet Derivatives

If the partial Fréchet derivatives xF(x0 , q0 ) and qF(x0 , q0 ) exist at the point z0 = p = ( x0 , q0 )T int[D( F )], , then we define the total derivative of F atp to be the continuous linear operator dzF(x0 , q0 ) : Z = Rn Rp ---> Rm given by

[dzF(p)]( , ) = [xF(x0 , q0 )]( ) + [qF(x0 , q0 )]( ).

Theorem D6. If F: D(F) Rn Rp ---> Rm is Fréchet differentiable at a point p = ( x0 , q0 )T int[D(F)], with derivative [DzF(p)]:Rn Rp ---> Rm , then both partial Fréchet derivatives exists at p and

[DzF(p)]( , ) = [dzF(p)]( , ) = [xF(x0 , q0 )]( ) + [qF(x0 , q0 )]( ).

Theorem D7. If the partial Fréchet derivatives xF(x0 , q0 ) and qF(x0 , q0 )exist and are continuous at each point in a neighborhood Rn Rp ofz0 = p = ( x0 , q0 )T int[D(F)], then F is Fréchet differentiable at the p and

[DzF(p)]( ,) = [xF(x0 , q0 )]( )+ [qF(x0 , q0 )]( ).

Page 61: THEORY OF ORDINARY DIFFERENTIAL EQUATIONS OF ORDINARY DIFFERENTIAL EQUATIONS Review of Advance Calculus Topics John A. Burns Center for Optimal Design And Control Interdisciplinary

Implicit Function Theorem

0 0( , ) 0F x q

Assume F : D(F) Rn Rp ---> Rn is a smooth function on a neighborhood ofz0 = [x0 , q0]T Rn Rp. If

and the partial Fréchet derivative

is one-to-one and onto Rn. Then there exists an open neighborhood Q of q0 and

a function such that

0 0( , ) : n nxF x q R R

: p nw Q R R

0 ) ( ) 0i w q and ) ( ( ), ) 0, for all .ii F w q q q Q

ˆ ˆ ˆ ˆ ˆ ˆ) [ ( ( ), )] [ ( )] [ ( ( ), )] 0, for all x q qiii F w q q D w q F w q q q Q

Moreover, the Fréchet derivative exists, is

continuous at each point , and

ˆ( )qD w q

q̂ Q

pR

nR

( )x w q

( , ) : ( , ) 0x q F x q