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MA 108 - Ordinary Differential Equations Santanu Dey Department of Mathematics, Indian Institute of Technology Bombay, Powai, Mumbai 76 [email protected] September 27, 2013 Santanu Dey Lecture 4

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Page 1: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

MA 108 - Ordinary Differential Equations

Santanu Dey

Department of Mathematics,Indian Institute of Technology Bombay,

Powai, Mumbai [email protected]

September 27, 2013

Santanu Dey Lecture 4

Page 2: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Outline of the lecture

Orthogonal Trajectories

Lipschitz continuity

Existence & uniqueness

Picard’s iteration

Santanu Dey Lecture 4

Page 3: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Solve : cos ydy

dx+

1

xsin y = 1.

Set v = sin y .

Then,

dv

dx=

dv

dy· dydx

= cos ydy

dx.

Hence the given equation is

dv

dx+

1

xv = 1, which is linear in v .

That is,

e∫

1xdxv(x) =

∫e∫

1xdxdx + C

=⇒ x v(x) =x2

2+ C

sin y =x

2+

C

x.

Santanu Dey Lecture 4

Page 4: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Solve : cos ydy

dx+

1

xsin y = 1.

Set v = sin y .Then,

dv

dx=

dv

dy· dydx

= cos ydy

dx.

Hence the given equation is

dv

dx+

1

xv = 1, which is linear in v .

That is,

e∫

1xdxv(x) =

∫e∫

1xdxdx + C

=⇒ x v(x) =x2

2+ C

sin y =x

2+

C

x.

Santanu Dey Lecture 4

Page 5: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Solve : cos ydy

dx+

1

xsin y = 1.

Set v = sin y .Then,

dv

dx=

dv

dy· dydx

=

cos ydy

dx.

Hence the given equation is

dv

dx+

1

xv = 1, which is linear in v .

That is,

e∫

1xdxv(x) =

∫e∫

1xdxdx + C

=⇒ x v(x) =x2

2+ C

sin y =x

2+

C

x.

Santanu Dey Lecture 4

Page 6: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Solve : cos ydy

dx+

1

xsin y = 1.

Set v = sin y .Then,

dv

dx=

dv

dy· dydx

= cos ydy

dx.

Hence the given equation is

dv

dx+

1

xv = 1, which is linear in v .

That is,

e∫

1xdxv(x) =

∫e∫

1xdxdx + C

=⇒ x v(x) =x2

2+ C

sin y =x

2+

C

x.

Santanu Dey Lecture 4

Page 7: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Solve : cos ydy

dx+

1

xsin y = 1.

Set v = sin y .Then,

dv

dx=

dv

dy· dydx

= cos ydy

dx.

Hence the given equation is

dv

dx+

1

xv = 1, which is linear in v .

That is,

e∫

1xdxv(x) =

∫e∫

1xdxdx + C

=⇒ x v(x) =x2

2+ C

sin y =x

2+

C

x.

Santanu Dey Lecture 4

Page 8: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Solve : cos ydy

dx+

1

xsin y = 1.

Set v = sin y .Then,

dv

dx=

dv

dy· dydx

= cos ydy

dx.

Hence the given equation is

dv

dx+

1

xv = 1, which is linear in v .

That is,

e∫

1xdxv(x) =

∫e∫

1xdxdx + C

=⇒ x v(x) =x2

2+ C

sin y =x

2+

C

x.

Santanu Dey Lecture 4

Page 9: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Solve : cos ydy

dx+

1

xsin y = 1.

Set v = sin y .Then,

dv

dx=

dv

dy· dydx

= cos ydy

dx.

Hence the given equation is

dv

dx+

1

xv = 1, which is linear in v .

That is,

e∫

1xdxv(x) =

∫e∫

1xdxdx + C

=⇒ x v(x) =x2

2+ C

sin y =x

2+

C

x.

Santanu Dey Lecture 4

Page 10: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Solve : cos ydy

dx+

1

xsin y = 1.

Set v = sin y .Then,

dv

dx=

dv

dy· dydx

= cos ydy

dx.

Hence the given equation is

dv

dx+

1

xv = 1, which is linear in v .

That is,

e∫

1xdxv(x) =

∫e∫

1xdxdx + C

=⇒ x v(x) =x2

2+ C

sin y =x

2+

C

x.

Santanu Dey Lecture 4

Page 11: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Orthogonal Trajectories

If two families of curves always intersect each other at right angles,then they are said to be orthogonal trajectories of each other.

Santanu Dey Lecture 4

Page 12: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Orthogonal Trajectories

If two families of curves always intersect each other at right angles,then they are said to be orthogonal trajectories of each other.

Santanu Dey Lecture 4

Page 13: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Working Rule

To find the OT of a family of curves

F (x , y , c) = 0.

Find the DEdy

dx= f (x , y).

Slopes of the OT’s are given by

dy

dx= − 1

f (x , y).

Obtain a one parameter family of curves G (x , y , c) = 0 assolutions of the above DE.

( Leaving a part certain trajectories that are vertical lines!)

Santanu Dey Lecture 4

Page 14: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Working Rule

To find the OT of a family of curves

F (x , y , c) = 0.

Find the DEdy

dx= f (x , y).

Slopes of the OT’s are given by

dy

dx= − 1

f (x , y).

Obtain a one parameter family of curves G (x , y , c) = 0 assolutions of the above DE.

( Leaving a part certain trajectories that are vertical lines!)

Santanu Dey Lecture 4

Page 15: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Working Rule

To find the OT of a family of curves

F (x , y , c) = 0.

Find the DEdy

dx= f (x , y).

Slopes of the OT’s are given by

dy

dx= − 1

f (x , y).

Obtain a one parameter family of curves G (x , y , c) = 0 assolutions of the above DE.

( Leaving a part certain trajectories that are vertical lines!)

Santanu Dey Lecture 4

Page 16: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Working Rule

To find the OT of a family of curves

F (x , y , c) = 0.

Find the DEdy

dx= f (x , y).

Slopes of the OT’s are given by

dy

dx= − 1

f (x , y).

Obtain a one parameter family of curves G (x , y , c) = 0 assolutions of the above DE.

( Leaving a part certain trajectories that are vertical lines!)

Santanu Dey Lecture 4

Page 17: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Working Rule

To find the OT of a family of curves

F (x , y , c) = 0.

Find the DEdy

dx= f (x , y).

Slopes of the OT’s are given by

dy

dx= − 1

f (x , y).

Obtain a one parameter family of curves G (x , y , c) = 0 assolutions of the above DE.

( Leaving a part certain trajectories that are vertical lines!)

Santanu Dey Lecture 4

Page 18: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Find the set of OT’s of the family of circles x2 + y2 = c2.

x + ydy

dx= 0 =⇒ dy

dx= −x

y

The slope of OT’s aredy

dx=

y

x=⇒ y = kx .

Hence the orthogonal trajectories are given by y = kx .

Santanu Dey Lecture 4

Page 19: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Find the set of OT’s of the family of circles x2 + y2 = c2.

x + ydy

dx= 0

=⇒ dy

dx= −x

y

The slope of OT’s aredy

dx=

y

x=⇒ y = kx .

Hence the orthogonal trajectories are given by y = kx .

Santanu Dey Lecture 4

Page 20: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Find the set of OT’s of the family of circles x2 + y2 = c2.

x + ydy

dx= 0 =⇒ dy

dx= −x

y

The slope of OT’s aredy

dx=

y

x=⇒ y = kx .

Hence the orthogonal trajectories are given by y = kx .

Santanu Dey Lecture 4

Page 21: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Find the set of OT’s of the family of circles x2 + y2 = c2.

x + ydy

dx= 0 =⇒ dy

dx= −x

y

The slope of OT’s are

dy

dx=

y

x=⇒ y = kx .

Hence the orthogonal trajectories are given by y = kx .

Santanu Dey Lecture 4

Page 22: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Find the set of OT’s of the family of circles x2 + y2 = c2.

x + ydy

dx= 0 =⇒ dy

dx= −x

y

The slope of OT’s aredy

dx=

y

x

=⇒ y = kx .

Hence the orthogonal trajectories are given by y = kx .

Santanu Dey Lecture 4

Page 23: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Find the set of OT’s of the family of circles x2 + y2 = c2.

x + ydy

dx= 0 =⇒ dy

dx= −x

y

The slope of OT’s aredy

dx=

y

x=⇒ y = kx .

Hence the orthogonal trajectories are given by y = kx .

Santanu Dey Lecture 4

Page 24: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Find the set of OT’s of the family of circles x2 + y2 = c2.

x + ydy

dx= 0 =⇒ dy

dx= −x

y

The slope of OT’s aredy

dx=

y

x=⇒ y = kx .

Hence the orthogonal trajectories are given by y = kx .

Santanu Dey Lecture 4

Page 25: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Definitions

1 Let f be a real function defined on D, where D is either adomain or a closed domain of the xy plane. The function f issaid to be bounded in D if there exists a positive number Msuch that

|f (x , y)| ≤ M

for all (x , y) in D.

2 Let f be defined and continuous on a closed rectangleR : a ≤ x ≤ b, c ≤ y ≤ d . Then, f is bounded in R.

3 Let f be defined on D, where D is either a domain or a closeddomain of the xy - plane. The function f is said to satisfyLipschitz condition (with respect to y) in D if ∃ a constantM > 0 such that

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2|

for every (x , y1), (x , y2) which belong to D. The constant Mis called the Lipschitz constant.

Santanu Dey Lecture 4

Page 26: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Definitions

1 Let f be a real function defined on D, where D is either adomain or a closed domain of the xy plane. The function f issaid to be bounded in D if there exists a positive number Msuch that

|f (x , y)| ≤ M

for all (x , y) in D.2 Let f be defined and continuous on a closed rectangle

R : a ≤ x ≤ b, c ≤ y ≤ d .

Then, f is bounded in R.3 Let f be defined on D, where D is either a domain or a closed

domain of the xy - plane. The function f is said to satisfyLipschitz condition (with respect to y) in D if ∃ a constantM > 0 such that

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2|

for every (x , y1), (x , y2) which belong to D. The constant Mis called the Lipschitz constant.

Santanu Dey Lecture 4

Page 27: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Definitions

1 Let f be a real function defined on D, where D is either adomain or a closed domain of the xy plane. The function f issaid to be bounded in D if there exists a positive number Msuch that

|f (x , y)| ≤ M

for all (x , y) in D.2 Let f be defined and continuous on a closed rectangle

R : a ≤ x ≤ b, c ≤ y ≤ d . Then, f is bounded in R.

3 Let f be defined on D, where D is either a domain or a closeddomain of the xy - plane. The function f is said to satisfyLipschitz condition (with respect to y) in D if ∃ a constantM > 0 such that

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2|

for every (x , y1), (x , y2) which belong to D. The constant Mis called the Lipschitz constant.

Santanu Dey Lecture 4

Page 28: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Definitions

1 Let f be a real function defined on D, where D is either adomain or a closed domain of the xy plane. The function f issaid to be bounded in D if there exists a positive number Msuch that

|f (x , y)| ≤ M

for all (x , y) in D.2 Let f be defined and continuous on a closed rectangle

R : a ≤ x ≤ b, c ≤ y ≤ d . Then, f is bounded in R.3 Let f be defined on D, where D is either a domain or a closed

domain of the xy - plane. The function f is said to satisfyLipschitz condition (with respect to y) in D if ∃ a constantM > 0 such that

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2|

for every (x , y1), (x , y2) which belong to D. The constant Mis called the Lipschitz constant.

Santanu Dey Lecture 4

Page 29: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Definitions

1 Let f be a real function defined on D, where D is either adomain or a closed domain of the xy plane. The function f issaid to be bounded in D if there exists a positive number Msuch that

|f (x , y)| ≤ M

for all (x , y) in D.2 Let f be defined and continuous on a closed rectangle

R : a ≤ x ≤ b, c ≤ y ≤ d . Then, f is bounded in R.3 Let f be defined on D, where D is either a domain or a closed

domain of the xy - plane. The function f is said to satisfyLipschitz condition (with respect to y) in D if ∃ a constantM > 0 such that

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2|

for every (x , y1), (x , y2) which belong to D. The constant Mis called the Lipschitz constant.

Santanu Dey Lecture 4

Page 30: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Definitions

1 Let f be a real function defined on D, where D is either adomain or a closed domain of the xy plane. The function f issaid to be bounded in D if there exists a positive number Msuch that

|f (x , y)| ≤ M

for all (x , y) in D.2 Let f be defined and continuous on a closed rectangle

R : a ≤ x ≤ b, c ≤ y ≤ d . Then, f is bounded in R.3 Let f be defined on D, where D is either a domain or a closed

domain of the xy - plane. The function f is said to satisfyLipschitz condition (with respect to y) in D if ∃ a constantM > 0 such that

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2|

for every (x , y1), (x , y2) which belong to D. The constant Mis called the Lipschitz constant.

Santanu Dey Lecture 4

Page 31: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Definitions

1 Let f be a real function defined on D, where D is either adomain or a closed domain of the xy plane. The function f issaid to be bounded in D if there exists a positive number Msuch that

|f (x , y)| ≤ M

for all (x , y) in D.2 Let f be defined and continuous on a closed rectangle

R : a ≤ x ≤ b, c ≤ y ≤ d . Then, f is bounded in R.3 Let f be defined on D, where D is either a domain or a closed

domain of the xy - plane. The function f is said to satisfyLipschitz condition (with respect to y) in D if ∃ a constantM > 0 such that

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2|

for every (x , y1), (x , y2) which belong to D. The constant Mis called the Lipschitz constant.

Santanu Dey Lecture 4

Page 32: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Understanding the Lipschitz condition - y = g(x)

Consider

|g(x2)− g(x1)| ≤ M|x2 − x1| ∀x1, x2 in the domain of g .

This condition in the form|g(x2)− g(x1)||x2 − x1|

≤ M can be interpreted

as follows :At each point (a, g(a)), the entire graph of g lies between the lines

y = g(a)−M(x − a) &y = g(a) + M(x − a).

Example : x2 is Lipschitz in [1, 2].

Santanu Dey Lecture 4

Page 33: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Understanding the Lipschitz condition - y = g(x)

Consider

|g(x2)− g(x1)| ≤ M|x2 − x1| ∀x1, x2 in the domain of g .

This condition in the form|g(x2)− g(x1)||x2 − x1|

≤ M can be interpreted

as follows :

At each point (a, g(a)), the entire graph of g lies between the lines

y = g(a)−M(x − a) &y = g(a) + M(x − a).

Example : x2 is Lipschitz in [1, 2].

Santanu Dey Lecture 4

Page 34: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Understanding the Lipschitz condition - y = g(x)

Consider

|g(x2)− g(x1)| ≤ M|x2 − x1| ∀x1, x2 in the domain of g .

This condition in the form|g(x2)− g(x1)||x2 − x1|

≤ M can be interpreted

as follows :At each point (a, g(a)), the entire graph of g lies between the lines

y = g(a)−M(x − a) &y = g(a) + M(x − a).

Example : x2 is Lipschitz in [1, 2].

Santanu Dey Lecture 4

Page 35: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Understanding the Lipschitz condition - y = g(x)

Consider

|g(x2)− g(x1)| ≤ M|x2 − x1| ∀x1, x2 in the domain of g .

This condition in the form|g(x2)− g(x1)||x2 − x1|

≤ M can be interpreted

as follows :At each point (a, g(a)), the entire graph of g lies between the lines

y = g(a)−M(x − a) &y = g(a) + M(x − a).

Example : x2 is Lipschitz in [1, 2].Santanu Dey Lecture 4

Page 36: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Understanding Lipschitz condition - z = f (x , y)

Let (x , y1) and (x , y2) be any two points in D having thesame abscissa x .

Consider the corresponding points

P1(x , y1, f (x , y1)) & P2(x , y2, f (x , y2))

on the surface z = f (x , y), and let α (0 ≤ α ≤ π/2) denotethe angle that the chord joining P1 and P2 makes with thexy - plane.

Then if the condition

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2|

holds in D, then tanα is bounded in absolute value.

That is, the chord joining P1 and P2 is bounded away frombeing perpendicular to the xy - plane.

Further, this bound is independent of the points (x , y1) and(x , y2) belonging to D.

Santanu Dey Lecture 4

Page 37: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Understanding Lipschitz condition - z = f (x , y)

Let (x , y1) and (x , y2) be any two points in D having thesame abscissa x .

Consider the corresponding points

P1(x , y1, f (x , y1)) & P2(x , y2, f (x , y2))

on the surface z = f (x , y), and let α (0 ≤ α ≤ π/2) denotethe angle that the chord joining P1 and P2 makes with thexy - plane.

Then if the condition

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2|

holds in D, then tanα is bounded in absolute value.

That is, the chord joining P1 and P2 is bounded away frombeing perpendicular to the xy - plane.

Further, this bound is independent of the points (x , y1) and(x , y2) belonging to D.

Santanu Dey Lecture 4

Page 38: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Understanding Lipschitz condition - z = f (x , y)

Let (x , y1) and (x , y2) be any two points in D having thesame abscissa x .

Consider the corresponding points

P1(x , y1, f (x , y1)) & P2(x , y2, f (x , y2))

on the surface z = f (x , y), and let α (0 ≤ α ≤ π/2) denotethe angle that the chord joining P1 and P2 makes with thexy - plane.

Then if the condition

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2|

holds in D, then tanα is bounded in absolute value.

That is, the chord joining P1 and P2 is bounded away frombeing perpendicular to the xy - plane.

Further, this bound is independent of the points (x , y1) and(x , y2) belonging to D.

Santanu Dey Lecture 4

Page 39: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Understanding Lipschitz condition - z = f (x , y)

Let (x , y1) and (x , y2) be any two points in D having thesame abscissa x .

Consider the corresponding points

P1(x , y1, f (x , y1)) & P2(x , y2, f (x , y2))

on the surface z = f (x , y), and let α (0 ≤ α ≤ π/2) denotethe angle that the chord joining P1 and P2 makes with thexy - plane.

Then if the condition

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2|

holds in D, then tanα is bounded in absolute value.

That is, the chord joining P1 and P2 is bounded away frombeing perpendicular to the xy - plane.

Further, this bound is independent of the points (x , y1) and(x , y2) belonging to D.

Santanu Dey Lecture 4

Page 40: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Understanding Lipschitz condition - z = f (x , y)

Let (x , y1) and (x , y2) be any two points in D having thesame abscissa x .

Consider the corresponding points

P1(x , y1, f (x , y1)) & P2(x , y2, f (x , y2))

on the surface z = f (x , y), and let α (0 ≤ α ≤ π/2) denotethe angle that the chord joining P1 and P2 makes with thexy - plane.

Then if the condition

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2|

holds in D, then tanα is bounded in absolute value.

That is, the chord joining P1 and P2 is bounded away frombeing perpendicular to the xy - plane.

Further, this bound is independent of the points (x , y1) and(x , y2) belonging to D.

Santanu Dey Lecture 4

Page 41: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Lipschitz condition =⇒ Continuity ?

If f satisfies Lipschitz condition with respect to y in D, then foreach fixed x , the resulting function of y is a continuous function ofy , for all (x , y) in D.

Example : Let f (x , y) = y + [x ].

For fixed x ,

f (x , y1)− f (x , y2) = y1 + [x ]− y2 − [x ]

= y1 − y2

That is, |f (x , y1)− f (x , y2)| = |y1 − y2| ≤ 1 · |y1 − y2|But we know that f is discontinuous w.r.t. x for every integralvalue of x .

Note that the condition of Lipschitz continuity implies nothing con-cerning the continuity of f with respect to x .

Santanu Dey Lecture 4

Page 42: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Lipschitz condition =⇒ Continuity ?

If f satisfies Lipschitz condition with respect to y in D, then foreach fixed x , the resulting function of y is a continuous function ofy , for all (x , y) in D.

Example : Let f (x , y) = y + [x ].

For fixed x ,

f (x , y1)− f (x , y2) = y1 + [x ]− y2 − [x ]

= y1 − y2

That is, |f (x , y1)− f (x , y2)| = |y1 − y2| ≤ 1 · |y1 − y2|But we know that f is discontinuous w.r.t. x for every integralvalue of x .

Note that the condition of Lipschitz continuity implies nothing con-cerning the continuity of f with respect to x .

Santanu Dey Lecture 4

Page 43: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Lipschitz condition =⇒ Continuity ?

If f satisfies Lipschitz condition with respect to y in D, then foreach fixed x , the resulting function of y is a continuous function ofy , for all (x , y) in D.

Example : Let f (x , y) = y + [x ].

For fixed x ,

f (x , y1)− f (x , y2) = y1 + [x ]− y2 − [x ]

= y1 − y2

That is, |f (x , y1)− f (x , y2)| = |y1 − y2| ≤ 1 · |y1 − y2|But we know that f is discontinuous w.r.t. x for every integralvalue of x .

Note that the condition of Lipschitz continuity implies nothing con-cerning the continuity of f with respect to x .

Santanu Dey Lecture 4

Page 44: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Lipschitz condition =⇒ Continuity ?

If f satisfies Lipschitz condition with respect to y in D, then foreach fixed x , the resulting function of y is a continuous function ofy , for all (x , y) in D.

Example : Let f (x , y) = y + [x ].

For fixed x ,

f (x , y1)− f (x , y2)

= y1 + [x ]− y2 − [x ]

= y1 − y2

That is, |f (x , y1)− f (x , y2)| = |y1 − y2| ≤ 1 · |y1 − y2|But we know that f is discontinuous w.r.t. x for every integralvalue of x .

Note that the condition of Lipschitz continuity implies nothing con-cerning the continuity of f with respect to x .

Santanu Dey Lecture 4

Page 45: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Lipschitz condition =⇒ Continuity ?

If f satisfies Lipschitz condition with respect to y in D, then foreach fixed x , the resulting function of y is a continuous function ofy , for all (x , y) in D.

Example : Let f (x , y) = y + [x ].

For fixed x ,

f (x , y1)− f (x , y2) = y1 + [x ]− y2 − [x ]

= y1 − y2

That is, |f (x , y1)− f (x , y2)| = |y1 − y2| ≤ 1 · |y1 − y2|But we know that f is discontinuous w.r.t. x for every integralvalue of x .

Note that the condition of Lipschitz continuity implies nothing con-cerning the continuity of f with respect to x .

Santanu Dey Lecture 4

Page 46: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Lipschitz condition =⇒ Continuity ?

If f satisfies Lipschitz condition with respect to y in D, then foreach fixed x , the resulting function of y is a continuous function ofy , for all (x , y) in D.

Example : Let f (x , y) = y + [x ].

For fixed x ,

f (x , y1)− f (x , y2) = y1 + [x ]− y2 − [x ]

= y1 − y2

That is, |f (x , y1)− f (x , y2)| = |y1 − y2| ≤ 1 · |y1 − y2|But we know that f is discontinuous w.r.t. x for every integralvalue of x .

Note that the condition of Lipschitz continuity implies nothing con-cerning the continuity of f with respect to x .

Santanu Dey Lecture 4

Page 47: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Lipschitz condition =⇒ Continuity ?

If f satisfies Lipschitz condition with respect to y in D, then foreach fixed x , the resulting function of y is a continuous function ofy , for all (x , y) in D.

Example : Let f (x , y) = y + [x ].

For fixed x ,

f (x , y1)− f (x , y2) = y1 + [x ]− y2 − [x ]

= y1 − y2

That is, |f (x , y1)− f (x , y2)| = |y1 − y2|

≤ 1 · |y1 − y2|But we know that f is discontinuous w.r.t. x for every integralvalue of x .

Note that the condition of Lipschitz continuity implies nothing con-cerning the continuity of f with respect to x .

Santanu Dey Lecture 4

Page 48: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Lipschitz condition =⇒ Continuity ?

If f satisfies Lipschitz condition with respect to y in D, then foreach fixed x , the resulting function of y is a continuous function ofy , for all (x , y) in D.

Example : Let f (x , y) = y + [x ].

For fixed x ,

f (x , y1)− f (x , y2) = y1 + [x ]− y2 − [x ]

= y1 − y2

That is, |f (x , y1)− f (x , y2)| = |y1 − y2| ≤ 1 · |y1 − y2|

But we know that f is discontinuous w.r.t. x for every integralvalue of x .

Note that the condition of Lipschitz continuity implies nothing con-cerning the continuity of f with respect to x .

Santanu Dey Lecture 4

Page 49: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Lipschitz condition =⇒ Continuity ?

If f satisfies Lipschitz condition with respect to y in D, then foreach fixed x , the resulting function of y is a continuous function ofy , for all (x , y) in D.

Example : Let f (x , y) = y + [x ].

For fixed x ,

f (x , y1)− f (x , y2) = y1 + [x ]− y2 − [x ]

= y1 − y2

That is, |f (x , y1)− f (x , y2)| = |y1 − y2| ≤ 1 · |y1 − y2|But we know that f is discontinuous w.r.t. x for every integralvalue of x .

Note that the condition of Lipschitz continuity implies nothing con-cerning the continuity of f with respect to x .

Santanu Dey Lecture 4

Page 50: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Lipschitz condition =⇒ Continuity ?

If f satisfies Lipschitz condition with respect to y in D, then foreach fixed x , the resulting function of y is a continuous function ofy , for all (x , y) in D.

Example : Let f (x , y) = y + [x ].

For fixed x ,

f (x , y1)− f (x , y2) = y1 + [x ]− y2 − [x ]

= y1 − y2

That is, |f (x , y1)− f (x , y2)| = |y1 − y2| ≤ 1 · |y1 − y2|But we know that f is discontinuous w.r.t. x for every integralvalue of x .

Note that the condition of Lipschitz continuity implies nothing con-cerning the continuity of f with respect to x .

Santanu Dey Lecture 4

Page 51: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Does Continuity w.r.t. second variable =⇒ Lipschitzcondtn. w.r.t. second variable?

Continuity w.r.t. second variable DOES NOT imply Lipschitzcondtn. w.r.t. second variable.

Example : Consider f (x , y) =√|y |.

f is continuous for all y .Note that f doesn’t satisfy Lipschitz condition in any region thatincludes y = 0 as for y1 = 0, y2 > 0, we have

|f (x , y1)− f (x , y2)||y1 − y2|

=

√y2|y2|

=1√y2

which can be made as large as we want by making y2 smaller.The Lipschitz condition requires that the quotient should bebounded by a fixed constant K .

Santanu Dey Lecture 4

Page 52: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Does Continuity w.r.t. second variable =⇒ Lipschitzcondtn. w.r.t. second variable?

Continuity w.r.t. second variable DOES NOT imply Lipschitzcondtn. w.r.t. second variable.

Example : Consider f (x , y) =√|y |.

f is continuous for all y .Note that f doesn’t satisfy Lipschitz condition in any region thatincludes y = 0 as for y1 = 0, y2 > 0, we have

|f (x , y1)− f (x , y2)||y1 − y2|

=

√y2|y2|

=1√y2

which can be made as large as we want by making y2 smaller.The Lipschitz condition requires that the quotient should bebounded by a fixed constant K .

Santanu Dey Lecture 4

Page 53: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Does Continuity w.r.t. second variable =⇒ Lipschitzcondtn. w.r.t. second variable?

Continuity w.r.t. second variable DOES NOT imply Lipschitzcondtn. w.r.t. second variable.

Example : Consider f (x , y) =√|y |.

f is continuous for all y .

Note that f doesn’t satisfy Lipschitz condition in any region thatincludes y = 0 as for y1 = 0, y2 > 0, we have

|f (x , y1)− f (x , y2)||y1 − y2|

=

√y2|y2|

=1√y2

which can be made as large as we want by making y2 smaller.The Lipschitz condition requires that the quotient should bebounded by a fixed constant K .

Santanu Dey Lecture 4

Page 54: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Does Continuity w.r.t. second variable =⇒ Lipschitzcondtn. w.r.t. second variable?

Continuity w.r.t. second variable DOES NOT imply Lipschitzcondtn. w.r.t. second variable.

Example : Consider f (x , y) =√|y |.

f is continuous for all y .Note that f doesn’t satisfy Lipschitz condition in any region thatincludes y = 0 as for y1 = 0, y2 > 0, we have

|f (x , y1)− f (x , y2)||y1 − y2|

=

√y2|y2|

=1√y2

which can be made as large as we want by making y2 smaller.The Lipschitz condition requires that the quotient should bebounded by a fixed constant K .

Santanu Dey Lecture 4

Page 55: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Does Continuity w.r.t. second variable =⇒ Lipschitzcondtn. w.r.t. second variable?

Continuity w.r.t. second variable DOES NOT imply Lipschitzcondtn. w.r.t. second variable.

Example : Consider f (x , y) =√|y |.

f is continuous for all y .Note that f doesn’t satisfy Lipschitz condition in any region thatincludes y = 0 as for y1 = 0, y2 > 0, we have

|f (x , y1)− f (x , y2)||y1 − y2|

=

√y2|y2|

=1√y2

which can be made as large as we want by making y2 smaller.The Lipschitz condition requires that the quotient should bebounded by a fixed constant K .

Santanu Dey Lecture 4

Page 56: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Does Continuity w.r.t. second variable =⇒ Lipschitzcondtn. w.r.t. second variable?

Continuity w.r.t. second variable DOES NOT imply Lipschitzcondtn. w.r.t. second variable.

Example : Consider f (x , y) =√|y |.

f is continuous for all y .Note that f doesn’t satisfy Lipschitz condition in any region thatincludes y = 0 as for y1 = 0, y2 > 0, we have

|f (x , y1)− f (x , y2)||y1 − y2|

=

√y2|y2|

=1√y2

which can be made as large as we want by making y2 smaller.The Lipschitz condition requires that the quotient should bebounded by a fixed constant K .

Santanu Dey Lecture 4

Page 57: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Does Continuity w.r.t. second variable =⇒ Lipschitzcondtn. w.r.t. second variable?

Continuity w.r.t. second variable DOES NOT imply Lipschitzcondtn. w.r.t. second variable.

Example : Consider f (x , y) =√|y |.

f is continuous for all y .Note that f doesn’t satisfy Lipschitz condition in any region thatincludes y = 0 as for y1 = 0, y2 > 0, we have

|f (x , y1)− f (x , y2)||y1 − y2|

=

√y2|y2|

=1√y2

which can be made as large as we want by making y2 smaller.The Lipschitz condition requires that the quotient should bebounded by a fixed constant K .

Santanu Dey Lecture 4

Page 58: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Does Continuity w.r.t. second variable =⇒ Lipschitzcondtn. w.r.t. second variable?

Continuity w.r.t. second variable DOES NOT imply Lipschitzcondtn. w.r.t. second variable.

Example : Consider f (x , y) =√|y |.

f is continuous for all y .Note that f doesn’t satisfy Lipschitz condition in any region thatincludes y = 0 as for y1 = 0, y2 > 0, we have

|f (x , y1)− f (x , y2)||y1 − y2|

=

√y2|y2|

=1√y2

which can be made as large as we want by making y2 smaller.

The Lipschitz condition requires that the quotient should bebounded by a fixed constant K .

Santanu Dey Lecture 4

Page 59: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Does Continuity w.r.t. second variable =⇒ Lipschitzcondtn. w.r.t. second variable?

Continuity w.r.t. second variable DOES NOT imply Lipschitzcondtn. w.r.t. second variable.

Example : Consider f (x , y) =√|y |.

f is continuous for all y .Note that f doesn’t satisfy Lipschitz condition in any region thatincludes y = 0 as for y1 = 0, y2 > 0, we have

|f (x , y1)− f (x , y2)||y1 − y2|

=

√y2|y2|

=1√y2

which can be made as large as we want by making y2 smaller.The Lipschitz condition requires that the quotient should bebounded by a fixed constant K .

Santanu Dey Lecture 4

Page 60: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Sufficiency

Result : If f is such that∂f

∂yexists and is bounded for all

(x , y) ∈ D, then f satisfies Lipschitz condition w.r.t. y in D, wherethe Lipschitz constant

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

Proof : Mean value theorem

=⇒ f (x , y1)− f (x , y2) = (y1 − y2)∂f

∂y(x , ξ), ξ ∈ (y1, y2).

|f (x , y1)− f (x , y2)| = |y1 − y2||∂f

∂y(x , ξ)|

≤ |y1 − y2| l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

That is, f satisfies Lipschitz condition.

Santanu Dey Lecture 4

Page 61: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Sufficiency

Result : If f is such that∂f

∂yexists and is bounded for all

(x , y) ∈ D, then f satisfies Lipschitz condition w.r.t. y in D, wherethe Lipschitz constant

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

Proof : Mean value theorem

=⇒

f (x , y1)− f (x , y2) = (y1 − y2)∂f

∂y(x , ξ), ξ ∈ (y1, y2).

|f (x , y1)− f (x , y2)| = |y1 − y2||∂f

∂y(x , ξ)|

≤ |y1 − y2| l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

That is, f satisfies Lipschitz condition.

Santanu Dey Lecture 4

Page 62: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Sufficiency

Result : If f is such that∂f

∂yexists and is bounded for all

(x , y) ∈ D, then f satisfies Lipschitz condition w.r.t. y in D, wherethe Lipschitz constant

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

Proof : Mean value theorem

=⇒ f (x , y1)− f (x , y2) = (y1 − y2)∂f

∂y(x , ξ),

ξ ∈ (y1, y2).

|f (x , y1)− f (x , y2)| = |y1 − y2||∂f

∂y(x , ξ)|

≤ |y1 − y2| l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

That is, f satisfies Lipschitz condition.

Santanu Dey Lecture 4

Page 63: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Sufficiency

Result : If f is such that∂f

∂yexists and is bounded for all

(x , y) ∈ D, then f satisfies Lipschitz condition w.r.t. y in D, wherethe Lipschitz constant

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

Proof : Mean value theorem

=⇒ f (x , y1)− f (x , y2) = (y1 − y2)∂f

∂y(x , ξ), ξ ∈ (y1, y2).

|f (x , y1)− f (x , y2)| = |y1 − y2||∂f

∂y(x , ξ)|

≤ |y1 − y2| l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

That is, f satisfies Lipschitz condition.

Santanu Dey Lecture 4

Page 64: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Sufficiency

Result : If f is such that∂f

∂yexists and is bounded for all

(x , y) ∈ D, then f satisfies Lipschitz condition w.r.t. y in D, wherethe Lipschitz constant

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

Proof : Mean value theorem

=⇒ f (x , y1)− f (x , y2) = (y1 − y2)∂f

∂y(x , ξ), ξ ∈ (y1, y2).

|f (x , y1)− f (x , y2)|

= |y1 − y2||∂f

∂y(x , ξ)|

≤ |y1 − y2| l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

That is, f satisfies Lipschitz condition.

Santanu Dey Lecture 4

Page 65: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Sufficiency

Result : If f is such that∂f

∂yexists and is bounded for all

(x , y) ∈ D, then f satisfies Lipschitz condition w.r.t. y in D, wherethe Lipschitz constant

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

Proof : Mean value theorem

=⇒ f (x , y1)− f (x , y2) = (y1 − y2)∂f

∂y(x , ξ), ξ ∈ (y1, y2).

|f (x , y1)− f (x , y2)| = |y1 − y2||∂f

∂y(x , ξ)|

≤ |y1 − y2| l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

That is, f satisfies Lipschitz condition.

Santanu Dey Lecture 4

Page 66: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Sufficiency

Result : If f is such that∂f

∂yexists and is bounded for all

(x , y) ∈ D, then f satisfies Lipschitz condition w.r.t. y in D, wherethe Lipschitz constant

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

Proof : Mean value theorem

=⇒ f (x , y1)− f (x , y2) = (y1 − y2)∂f

∂y(x , ξ), ξ ∈ (y1, y2).

|f (x , y1)− f (x , y2)| = |y1 − y2||∂f

∂y(x , ξ)|

≤ |y1 − y2| l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

That is, f satisfies Lipschitz condition.

Santanu Dey Lecture 4

Page 67: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Sufficiency

Result : If f is such that∂f

∂yexists and is bounded for all

(x , y) ∈ D, then f satisfies Lipschitz condition w.r.t. y in D, wherethe Lipschitz constant

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

Proof : Mean value theorem

=⇒ f (x , y1)− f (x , y2) = (y1 − y2)∂f

∂y(x , ξ), ξ ∈ (y1, y2).

|f (x , y1)− f (x , y2)| = |y1 − y2||∂f

∂y(x , ξ)|

≤ |y1 − y2| l .u.b.(x ,y)∈D |∂f

∂y(x , y)|.

That is, f satisfies Lipschitz condition.

Santanu Dey Lecture 4

Page 68: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Consider

f (x , y) = y2 defined in D : |x | ≤ a, |y | ≤ b.

fy = 2y is bounded in D. The Lipschitz contant is

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)| = l .u.b.(x ,y)∈D |2y | = 2b.

(Verify Lipschitz condition directly! )

Santanu Dey Lecture 4

Page 69: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Consider

f (x , y) = y2 defined in D : |x | ≤ a, |y | ≤ b.

fy = 2y is bounded in D.

The Lipschitz contant is

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)| = l .u.b.(x ,y)∈D |2y | = 2b.

(Verify Lipschitz condition directly! )

Santanu Dey Lecture 4

Page 70: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Consider

f (x , y) = y2 defined in D : |x | ≤ a, |y | ≤ b.

fy = 2y is bounded in D. The Lipschitz contant is

M =

l .u.b.(x ,y)∈D |∂f

∂y(x , y)| = l .u.b.(x ,y)∈D |2y | = 2b.

(Verify Lipschitz condition directly! )

Santanu Dey Lecture 4

Page 71: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Consider

f (x , y) = y2 defined in D : |x | ≤ a, |y | ≤ b.

fy = 2y is bounded in D. The Lipschitz contant is

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)| =

l .u.b.(x ,y)∈D |2y | = 2b.

(Verify Lipschitz condition directly! )

Santanu Dey Lecture 4

Page 72: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Consider

f (x , y) = y2 defined in D : |x | ≤ a, |y | ≤ b.

fy = 2y is bounded in D. The Lipschitz contant is

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)| = l .u.b.(x ,y)∈D |2y |

= 2b.

(Verify Lipschitz condition directly! )

Santanu Dey Lecture 4

Page 73: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Consider

f (x , y) = y2 defined in D : |x | ≤ a, |y | ≤ b.

fy = 2y is bounded in D. The Lipschitz contant is

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)| = l .u.b.(x ,y)∈D |2y | = 2b.

(Verify Lipschitz condition directly! )

Santanu Dey Lecture 4

Page 74: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example

Consider

f (x , y) = y2 defined in D : |x | ≤ a, |y | ≤ b.

fy = 2y is bounded in D. The Lipschitz contant is

M = l .u.b.(x ,y)∈D |∂f

∂y(x , y)| = l .u.b.(x ,y)∈D |2y | = 2b.

(Verify Lipschitz condition directly! )

Santanu Dey Lecture 4

Page 75: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Bounded derivative - sufficient condition

Consider

f (x , y) = x |y | defined in D : |x | ≤ a, |y | ≤ b.

∂f

∂ydoesn’t exist for any point (x , 0) ∈ D. (Why?)

Now f satisfies Lipschitz condition :

|f (x , y1)− f (x , y2)| =∣∣x |y1| − x |y2|

∣∣= |x |

∣∣|y1| − |y2|∣∣≤ |x | |y1 − y2|≤ a|y1 − y2|

Existence of bounded derivative fy is a sufficient condition for Lips-chitz condition to hold true (not necessary).

Santanu Dey Lecture 4

Page 76: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Bounded derivative - sufficient condition

Consider

f (x , y) = x |y | defined in D : |x | ≤ a, |y | ≤ b.

∂f

∂ydoesn’t exist for any point (x , 0) ∈ D.

(Why?)

Now f satisfies Lipschitz condition :

|f (x , y1)− f (x , y2)| =∣∣x |y1| − x |y2|

∣∣= |x |

∣∣|y1| − |y2|∣∣≤ |x | |y1 − y2|≤ a|y1 − y2|

Existence of bounded derivative fy is a sufficient condition for Lips-chitz condition to hold true (not necessary).

Santanu Dey Lecture 4

Page 77: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Bounded derivative - sufficient condition

Consider

f (x , y) = x |y | defined in D : |x | ≤ a, |y | ≤ b.

∂f

∂ydoesn’t exist for any point (x , 0) ∈ D. (Why?)

Now f satisfies Lipschitz condition :

|f (x , y1)− f (x , y2)| =∣∣x |y1| − x |y2|

∣∣= |x |

∣∣|y1| − |y2|∣∣≤ |x | |y1 − y2|≤ a|y1 − y2|

Existence of bounded derivative fy is a sufficient condition for Lips-chitz condition to hold true (not necessary).

Santanu Dey Lecture 4

Page 78: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Bounded derivative - sufficient condition

Consider

f (x , y) = x |y | defined in D : |x | ≤ a, |y | ≤ b.

∂f

∂ydoesn’t exist for any point (x , 0) ∈ D. (Why?)

Now f satisfies Lipschitz condition :

|f (x , y1)− f (x , y2)| =

∣∣x |y1| − x |y2|∣∣

= |x |∣∣|y1| − |y2|∣∣

≤ |x | |y1 − y2|≤ a|y1 − y2|

Existence of bounded derivative fy is a sufficient condition for Lips-chitz condition to hold true (not necessary).

Santanu Dey Lecture 4

Page 79: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Bounded derivative - sufficient condition

Consider

f (x , y) = x |y | defined in D : |x | ≤ a, |y | ≤ b.

∂f

∂ydoesn’t exist for any point (x , 0) ∈ D. (Why?)

Now f satisfies Lipschitz condition :

|f (x , y1)− f (x , y2)| =∣∣x |y1| − x |y2|

∣∣

= |x |∣∣|y1| − |y2|∣∣

≤ |x | |y1 − y2|≤ a|y1 − y2|

Existence of bounded derivative fy is a sufficient condition for Lips-chitz condition to hold true (not necessary).

Santanu Dey Lecture 4

Page 80: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Bounded derivative - sufficient condition

Consider

f (x , y) = x |y | defined in D : |x | ≤ a, |y | ≤ b.

∂f

∂ydoesn’t exist for any point (x , 0) ∈ D. (Why?)

Now f satisfies Lipschitz condition :

|f (x , y1)− f (x , y2)| =∣∣x |y1| − x |y2|

∣∣= |x |

∣∣|y1| − |y2|∣∣

≤ |x | |y1 − y2|≤ a|y1 − y2|

Existence of bounded derivative fy is a sufficient condition for Lips-chitz condition to hold true (not necessary).

Santanu Dey Lecture 4

Page 81: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Bounded derivative - sufficient condition

Consider

f (x , y) = x |y | defined in D : |x | ≤ a, |y | ≤ b.

∂f

∂ydoesn’t exist for any point (x , 0) ∈ D. (Why?)

Now f satisfies Lipschitz condition :

|f (x , y1)− f (x , y2)| =∣∣x |y1| − x |y2|

∣∣= |x |

∣∣|y1| − |y2|∣∣≤ |x | |y1 − y2|

≤ a|y1 − y2|

Existence of bounded derivative fy is a sufficient condition for Lips-chitz condition to hold true (not necessary).

Santanu Dey Lecture 4

Page 82: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Bounded derivative - sufficient condition

Consider

f (x , y) = x |y | defined in D : |x | ≤ a, |y | ≤ b.

∂f

∂ydoesn’t exist for any point (x , 0) ∈ D. (Why?)

Now f satisfies Lipschitz condition :

|f (x , y1)− f (x , y2)| =∣∣x |y1| − x |y2|

∣∣= |x |

∣∣|y1| − |y2|∣∣≤ |x | |y1 − y2|≤ a|y1 − y2|

Existence of bounded derivative fy is a sufficient condition for Lips-chitz condition to hold true (not necessary).

Santanu Dey Lecture 4

Page 83: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Bounded derivative - sufficient condition

Consider

f (x , y) = x |y | defined in D : |x | ≤ a, |y | ≤ b.

∂f

∂ydoesn’t exist for any point (x , 0) ∈ D. (Why?)

Now f satisfies Lipschitz condition :

|f (x , y1)− f (x , y2)| =∣∣x |y1| − x |y2|

∣∣= |x |

∣∣|y1| − |y2|∣∣≤ |x | |y1 − y2|≤ a|y1 − y2|

Existence of bounded derivative fy is a sufficient condition for Lips-chitz condition to hold true (not necessary).

Santanu Dey Lecture 4

Page 84: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Existence - Uniqueness Theorem

Let R be a rectangle containing (x0, y0) in the domain D,

f (x , y) be continuous at all points (x , y) inR : |x − x0| < a, |y − y0| < b and

bounded in R, that is, |f (x , y)| ≤ K ∀(x , y) ∈ R.

Then, the IVP y ′ = f (x , y), y(x0) = y0 has at least one solution y(x)

defined for all x in the interval |x − x0| < α, where

α = min

{a,

b

K

}.

In addition to the above conditions, if f satisfies the Lipschitz conditionwith respect to y in R, that is,

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2| ∀(x , y1), (x , y2) in R,

then, the solution y(x) defined at least for all x in the interval |x−x0| < α,with α defined above is unique 1.

1Existence - Peano, Existence & uniqueness -PicardSantanu Dey Lecture 4

Page 85: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Existence - Uniqueness Theorem

Let R be a rectangle containing (x0, y0) in the domain D,

f (x , y) be continuous at all points (x , y) inR : |x − x0| < a, |y − y0| < b and

bounded in R, that is, |f (x , y)| ≤ K ∀(x , y) ∈ R.

Then, the IVP y ′ = f (x , y), y(x0) = y0 has at least one solution y(x)

defined for all x in the interval |x − x0| < α, where

α = min

{a,

b

K

}.

In addition to the above conditions, if f satisfies the Lipschitz conditionwith respect to y in R, that is,

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2| ∀(x , y1), (x , y2) in R,

then, the solution y(x) defined at least for all x in the interval |x−x0| < α,with α defined above is unique 1.

1Existence - Peano, Existence & uniqueness -PicardSantanu Dey Lecture 4

Page 86: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Existence - Uniqueness Theorem

Let R be a rectangle containing (x0, y0) in the domain D,

f (x , y) be continuous at all points (x , y) inR : |x − x0| < a, |y − y0| < b and

bounded in R, that is, |f (x , y)| ≤ K ∀(x , y) ∈ R.

Then, the IVP y ′ = f (x , y), y(x0) = y0 has at least one solution y(x)

defined for all x in the interval |x − x0| < α, where

α = min

{a,

b

K

}.

In addition to the above conditions, if f satisfies the Lipschitz conditionwith respect to y in R, that is,

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2| ∀(x , y1), (x , y2) in R,

then, the solution y(x) defined at least for all x in the interval |x−x0| < α,with α defined above is unique 1.

1Existence - Peano, Existence & uniqueness -PicardSantanu Dey Lecture 4

Page 87: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Existence - Uniqueness Theorem

Let R be a rectangle containing (x0, y0) in the domain D,

f (x , y) be continuous at all points (x , y) inR : |x − x0| < a, |y − y0| < b and

bounded in R, that is, |f (x , y)| ≤ K ∀(x , y) ∈ R.

Then, the IVP y ′ = f (x , y), y(x0) = y0 has at least one solution y(x)

defined for all x in the interval |x − x0| < α, where

α = min

{a,

b

K

}.

In addition to the above conditions, if f satisfies the Lipschitz conditionwith respect to y in R, that is,

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2| ∀(x , y1), (x , y2) in R,

then, the solution y(x) defined at least for all x in the interval |x−x0| < α,with α defined above is unique 1.

1Existence - Peano, Existence & uniqueness -PicardSantanu Dey Lecture 4

Page 88: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Existence - Uniqueness Theorem

Let R be a rectangle containing (x0, y0) in the domain D,

f (x , y) be continuous at all points (x , y) inR : |x − x0| < a, |y − y0| < b and

bounded in R, that is, |f (x , y)| ≤ K ∀(x , y) ∈ R.

Then, the IVP y ′ = f (x , y), y(x0) = y0 has at least one solution y(x)

defined for all x in the interval |x − x0| < α, where

α = min

{a,

b

K

}.

In addition to the above conditions, if f satisfies the Lipschitz conditionwith respect to y in R, that is,

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2| ∀(x , y1), (x , y2) in R,

then, the solution y(x) defined at least for all x in the interval |x−x0| < α,with α defined above is unique 1.

1Existence - Peano, Existence & uniqueness -PicardSantanu Dey Lecture 4

Page 89: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Existence - Uniqueness Theorem

Let R be a rectangle containing (x0, y0) in the domain D,

f (x , y) be continuous at all points (x , y) inR : |x − x0| < a, |y − y0| < b and

bounded in R, that is, |f (x , y)| ≤ K ∀(x , y) ∈ R.

Then, the IVP y ′ = f (x , y), y(x0) = y0 has at least one solution y(x)

defined for all x in the interval |x − x0| < α, where

α = min

{a,

b

K

}.

In addition to the above conditions, if f satisfies the Lipschitz conditionwith respect to y in R, that is,

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2| ∀(x , y1), (x , y2) in R,

then, the solution y(x) defined at least for all x in the interval |x−x0| < α,with α defined above is unique 1.

1Existence - Peano, Existence & uniqueness -PicardSantanu Dey Lecture 4

Page 90: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Existence - Uniqueness Theorem

Let R be a rectangle containing (x0, y0) in the domain D,

f (x , y) be continuous at all points (x , y) inR : |x − x0| < a, |y − y0| < b and

bounded in R, that is, |f (x , y)| ≤ K ∀(x , y) ∈ R.

Then, the IVP y ′ = f (x , y), y(x0) = y0 has at least one solution y(x)

defined for all x in the interval |x − x0| < α, where

α = min

{a,

b

K

}.

In addition to the above conditions, if f satisfies the Lipschitz conditionwith respect to y in R, that is,

|f (x , y1)− f (x , y2)| ≤ M|y1 − y2| ∀(x , y1), (x , y2) in R,

then, the solution y(x) defined at least for all x in the interval |x−x0| < α,with α defined above is unique 1.

1Existence - Peano, Existence & uniqueness -PicardSantanu Dey Lecture 4

Page 91: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

A quick check!

1 Is f (x) = sin x Lipschitz continuous over R?

Yes.

2 Is f (x) = x2 globally Lipschitz continuous over R ? No.However, it is Lipschitz continuous over any closed interval ofR. We say that it is locally Lipschitz continuous over R.

3 Is f (x) =1

x2globally Lipschitz continuous on [α,∞) for any

α > 0? Yes.

Santanu Dey Lecture 4

Page 92: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

A quick check!

1 Is f (x) = sin x Lipschitz continuous over R? Yes.

2 Is f (x) = x2 globally Lipschitz continuous over R ?

No.However, it is Lipschitz continuous over any closed interval ofR. We say that it is locally Lipschitz continuous over R.

3 Is f (x) =1

x2globally Lipschitz continuous on [α,∞) for any

α > 0? Yes.

Santanu Dey Lecture 4

Page 93: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

A quick check!

1 Is f (x) = sin x Lipschitz continuous over R? Yes.

2 Is f (x) = x2 globally Lipschitz continuous over R ? No.

However, it is Lipschitz continuous over any closed interval ofR. We say that it is locally Lipschitz continuous over R.

3 Is f (x) =1

x2globally Lipschitz continuous on [α,∞) for any

α > 0? Yes.

Santanu Dey Lecture 4

Page 94: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

A quick check!

1 Is f (x) = sin x Lipschitz continuous over R? Yes.

2 Is f (x) = x2 globally Lipschitz continuous over R ? No.However, it is Lipschitz continuous over any closed interval ofR.

We say that it is locally Lipschitz continuous over R.

3 Is f (x) =1

x2globally Lipschitz continuous on [α,∞) for any

α > 0? Yes.

Santanu Dey Lecture 4

Page 95: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

A quick check!

1 Is f (x) = sin x Lipschitz continuous over R? Yes.

2 Is f (x) = x2 globally Lipschitz continuous over R ? No.However, it is Lipschitz continuous over any closed interval ofR. We say that it is locally Lipschitz continuous over R.

3 Is f (x) =1

x2globally Lipschitz continuous on [α,∞) for any

α > 0? Yes.

Santanu Dey Lecture 4

Page 96: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

A quick check!

1 Is f (x) = sin x Lipschitz continuous over R? Yes.

2 Is f (x) = x2 globally Lipschitz continuous over R ? No.However, it is Lipschitz continuous over any closed interval ofR. We say that it is locally Lipschitz continuous over R.

3 Is f (x) =1

x2globally Lipschitz continuous on [α,∞) for any

α > 0?

Yes.

Santanu Dey Lecture 4

Page 97: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

A quick check!

1 Is f (x) = sin x Lipschitz continuous over R? Yes.

2 Is f (x) = x2 globally Lipschitz continuous over R ? No.However, it is Lipschitz continuous over any closed interval ofR. We say that it is locally Lipschitz continuous over R.

3 Is f (x) =1

x2globally Lipschitz continuous on [α,∞) for any

α > 0? Yes.

Santanu Dey Lecture 4

Page 98: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

A quick check!

1 Is f (x) = sin x Lipschitz continuous over R? Yes.

2 Is f (x) = x2 globally Lipschitz continuous over R ? No.However, it is Lipschitz continuous over any closed interval ofR. We say that it is locally Lipschitz continuous over R.

3 Is f (x) =1

x2globally Lipschitz continuous on [α,∞) for any

α > 0? Yes.

Santanu Dey Lecture 4

Page 99: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 1

Consider

y ′ = y1/3 y(0) = 0 in R : |x | ≤ a, |y | ≤ b.

f (x , y) is continuous in R and hence existence is guaranteed.

But φ1(x) = 0 and φ2(x) =

(2

3x)3/2 if x ≥ 0

0 if x ≤ 0are solutions in

−∞ < x <∞.Does this imply Lipschitz condition won’t be satisfied?

|f (x , y1)− f (x , y2)||y1 − y2|

=|y1/31 − y

1/32 |

|y1 − y2|.

Choosing y1 = δ, y2 = −δ, we see that the quotient is unboundedfor small values of δ and hence Lipschitz condition is not satisfied.Solution exists, but not unique.

Santanu Dey Lecture 4

Page 100: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 1

Consider

y ′ = y1/3 y(0) = 0 in R : |x | ≤ a, |y | ≤ b.

f (x , y) is continuous in R and hence existence is guaranteed.

But φ1(x) = 0 and φ2(x) =

(2

3x)3/2 if x ≥ 0

0 if x ≤ 0are solutions in

−∞ < x <∞.Does this imply Lipschitz condition won’t be satisfied?

|f (x , y1)− f (x , y2)||y1 − y2|

=|y1/31 − y

1/32 |

|y1 − y2|.

Choosing y1 = δ, y2 = −δ, we see that the quotient is unboundedfor small values of δ and hence Lipschitz condition is not satisfied.Solution exists, but not unique.

Santanu Dey Lecture 4

Page 101: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 1

Consider

y ′ = y1/3 y(0) = 0 in R : |x | ≤ a, |y | ≤ b.

f (x , y) is continuous in R and hence existence is guaranteed.

But φ1(x) = 0

and φ2(x) =

(2

3x)3/2 if x ≥ 0

0 if x ≤ 0are solutions in

−∞ < x <∞.Does this imply Lipschitz condition won’t be satisfied?

|f (x , y1)− f (x , y2)||y1 − y2|

=|y1/31 − y

1/32 |

|y1 − y2|.

Choosing y1 = δ, y2 = −δ, we see that the quotient is unboundedfor small values of δ and hence Lipschitz condition is not satisfied.Solution exists, but not unique.

Santanu Dey Lecture 4

Page 102: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 1

Consider

y ′ = y1/3 y(0) = 0 in R : |x | ≤ a, |y | ≤ b.

f (x , y) is continuous in R and hence existence is guaranteed.

But φ1(x) = 0 and φ2(x) =

(2

3x)3/2 if x ≥ 0

0 if x ≤ 0are solutions in

−∞ < x <∞.

Does this imply Lipschitz condition won’t be satisfied?

|f (x , y1)− f (x , y2)||y1 − y2|

=|y1/31 − y

1/32 |

|y1 − y2|.

Choosing y1 = δ, y2 = −δ, we see that the quotient is unboundedfor small values of δ and hence Lipschitz condition is not satisfied.Solution exists, but not unique.

Santanu Dey Lecture 4

Page 103: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 1

Consider

y ′ = y1/3 y(0) = 0 in R : |x | ≤ a, |y | ≤ b.

f (x , y) is continuous in R and hence existence is guaranteed.

But φ1(x) = 0 and φ2(x) =

(2

3x)3/2 if x ≥ 0

0 if x ≤ 0are solutions in

−∞ < x <∞.Does this imply Lipschitz condition won’t be satisfied?

|f (x , y1)− f (x , y2)||y1 − y2|

=|y1/31 − y

1/32 |

|y1 − y2|.

Choosing y1 = δ, y2 = −δ, we see that the quotient is unboundedfor small values of δ and hence Lipschitz condition is not satisfied.Solution exists, but not unique.

Santanu Dey Lecture 4

Page 104: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 1

Consider

y ′ = y1/3 y(0) = 0 in R : |x | ≤ a, |y | ≤ b.

f (x , y) is continuous in R and hence existence is guaranteed.

But φ1(x) = 0 and φ2(x) =

(2

3x)3/2 if x ≥ 0

0 if x ≤ 0are solutions in

−∞ < x <∞.Does this imply Lipschitz condition won’t be satisfied?

|f (x , y1)− f (x , y2)||y1 − y2|

=

|y1/31 − y1/32 |

|y1 − y2|.

Choosing y1 = δ, y2 = −δ, we see that the quotient is unboundedfor small values of δ and hence Lipschitz condition is not satisfied.Solution exists, but not unique.

Santanu Dey Lecture 4

Page 105: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 1

Consider

y ′ = y1/3 y(0) = 0 in R : |x | ≤ a, |y | ≤ b.

f (x , y) is continuous in R and hence existence is guaranteed.

But φ1(x) = 0 and φ2(x) =

(2

3x)3/2 if x ≥ 0

0 if x ≤ 0are solutions in

−∞ < x <∞.Does this imply Lipschitz condition won’t be satisfied?

|f (x , y1)− f (x , y2)||y1 − y2|

=|y1/31 − y

1/32 |

|y1 − y2|.

Choosing y1 = δ, y2 = −δ, we see that the quotient is unboundedfor small values of δ and hence Lipschitz condition is not satisfied.Solution exists, but not unique.

Santanu Dey Lecture 4

Page 106: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 1

Consider

y ′ = y1/3 y(0) = 0 in R : |x | ≤ a, |y | ≤ b.

f (x , y) is continuous in R and hence existence is guaranteed.

But φ1(x) = 0 and φ2(x) =

(2

3x)3/2 if x ≥ 0

0 if x ≤ 0are solutions in

−∞ < x <∞.Does this imply Lipschitz condition won’t be satisfied?

|f (x , y1)− f (x , y2)||y1 − y2|

=|y1/31 − y

1/32 |

|y1 − y2|.

Choosing y1 = δ, y2 = −δ, we see that the quotient is unboundedfor small values of δ and hence Lipschitz condition is not satisfied.

Solution exists, but not unique.

Santanu Dey Lecture 4

Page 107: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 1

Consider

y ′ = y1/3 y(0) = 0 in R : |x | ≤ a, |y | ≤ b.

f (x , y) is continuous in R and hence existence is guaranteed.

But φ1(x) = 0 and φ2(x) =

(2

3x)3/2 if x ≥ 0

0 if x ≤ 0are solutions in

−∞ < x <∞.Does this imply Lipschitz condition won’t be satisfied?

|f (x , y1)− f (x , y2)||y1 − y2|

=|y1/31 − y

1/32 |

|y1 − y2|.

Choosing y1 = δ, y2 = −δ, we see that the quotient is unboundedfor small values of δ and hence Lipschitz condition is not satisfied.Solution exists, but not unique.

Santanu Dey Lecture 4

Page 108: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2

Consider y ′ = y2, y(1) = −1. Find α in the existence &uniqueness theorem.

(1,−1)

(1 − a,−1 − b) (1 + a,−1 − b)

(1 − a,−1 + b) (1 + a,−1 + b)

f (x , y) = y2, fy = 2y are continuous in the closed rectangleR : |x − 1| ≤ a, |y + 1| ≤ b.

|f (x , y)| = |y |2 ≤ |(−b − 1)|2 ≤ (b + 1)2 (1)

Now, α = min

{a,

b

(b + 1)2

}.

Santanu Dey Lecture 4

Page 109: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2

Consider y ′ = y2, y(1) = −1. Find α in the existence &uniqueness theorem.

(1,−1)

(1 − a,−1 − b) (1 + a,−1 − b)

(1 − a,−1 + b) (1 + a,−1 + b)

f (x , y) = y2, fy = 2y are continuous in the closed rectangleR : |x − 1| ≤ a, |y + 1| ≤ b.

|f (x , y)| = |y |2 ≤ |(−b − 1)|2 ≤ (b + 1)2 (1)

Now, α = min

{a,

b

(b + 1)2

}.

Santanu Dey Lecture 4

Page 110: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2

Consider y ′ = y2, y(1) = −1. Find α in the existence &uniqueness theorem.

(1,−1)

(1 − a,−1 − b) (1 + a,−1 − b)

(1 − a,−1 + b) (1 + a,−1 + b)

f (x , y) = y2, fy = 2y are continuous in the closed rectangleR : |x − 1| ≤ a, |y + 1| ≤ b.

|f (x , y)| = |y |2 ≤ |(−b − 1)|2 ≤ (b + 1)2 (1)

Now, α = min

{a,

b

(b + 1)2

}.

Santanu Dey Lecture 4

Page 111: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2

Consider y ′ = y2, y(1) = −1. Find α in the existence &uniqueness theorem.

(1,−1)

(1 − a,−1 − b) (1 + a,−1 − b)

(1 − a,−1 + b) (1 + a,−1 + b)

f (x , y) = y2, fy = 2y are continuous in the closed rectangleR : |x − 1| ≤ a, |y + 1| ≤ b.

|f (x , y)|

= |y |2 ≤ |(−b − 1)|2 ≤ (b + 1)2 (1)

Now, α = min

{a,

b

(b + 1)2

}.

Santanu Dey Lecture 4

Page 112: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2

Consider y ′ = y2, y(1) = −1. Find α in the existence &uniqueness theorem.

(1,−1)

(1 − a,−1 − b) (1 + a,−1 − b)

(1 − a,−1 + b) (1 + a,−1 + b)

f (x , y) = y2, fy = 2y are continuous in the closed rectangleR : |x − 1| ≤ a, |y + 1| ≤ b.

|f (x , y)| = |y |2

≤ |(−b − 1)|2 ≤ (b + 1)2 (1)

Now, α = min

{a,

b

(b + 1)2

}.

Santanu Dey Lecture 4

Page 113: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2

Consider y ′ = y2, y(1) = −1. Find α in the existence &uniqueness theorem.

(1,−1)

(1 − a,−1 − b) (1 + a,−1 − b)

(1 − a,−1 + b) (1 + a,−1 + b)

f (x , y) = y2, fy = 2y are continuous in the closed rectangleR : |x − 1| ≤ a, |y + 1| ≤ b.

|f (x , y)| = |y |2 ≤ |(−b − 1)|2

≤ (b + 1)2 (1)

Now, α = min

{a,

b

(b + 1)2

}.

Santanu Dey Lecture 4

Page 114: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2

Consider y ′ = y2, y(1) = −1. Find α in the existence &uniqueness theorem.

(1,−1)

(1 − a,−1 − b) (1 + a,−1 − b)

(1 − a,−1 + b) (1 + a,−1 + b)

f (x , y) = y2, fy = 2y are continuous in the closed rectangleR : |x − 1| ≤ a, |y + 1| ≤ b.

|f (x , y)| = |y |2 ≤ |(−b − 1)|2 ≤ (b + 1)2

(1)

Now, α = min

{a,

b

(b + 1)2

}.

Santanu Dey Lecture 4

Page 115: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2

Consider y ′ = y2, y(1) = −1. Find α in the existence &uniqueness theorem.

(1,−1)

(1 − a,−1 − b) (1 + a,−1 − b)

(1 − a,−1 + b) (1 + a,−1 + b)

f (x , y) = y2, fy = 2y are continuous in the closed rectangleR : |x − 1| ≤ a, |y + 1| ≤ b.

|f (x , y)| = |y |2 ≤ |(−b − 1)|2 ≤ (b + 1)2 (1)

Now, α =

min

{a,

b

(b + 1)2

}.

Santanu Dey Lecture 4

Page 116: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2

Consider y ′ = y2, y(1) = −1. Find α in the existence &uniqueness theorem.

(1,−1)

(1 − a,−1 − b) (1 + a,−1 − b)

(1 − a,−1 + b) (1 + a,−1 + b)

f (x , y) = y2, fy = 2y are continuous in the closed rectangleR : |x − 1| ≤ a, |y + 1| ≤ b.

|f (x , y)| = |y |2 ≤ |(−b − 1)|2 ≤ (b + 1)2 (1)

Now, α = min

{a,

b

(b + 1)2

}.

Santanu Dey Lecture 4

Page 117: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2

Consider y ′ = y2, y(1) = −1. Find α in the existence &uniqueness theorem.

(1,−1)

(1 − a,−1 − b) (1 + a,−1 − b)

(1 − a,−1 + b) (1 + a,−1 + b)

f (x , y) = y2, fy = 2y are continuous in the closed rectangleR : |x − 1| ≤ a, |y + 1| ≤ b.

|f (x , y)| = |y |2 ≤ |(−b − 1)|2 ≤ (b + 1)2 (1)

Now, α = min

{a,

b

(b + 1)2

}.

Santanu Dey Lecture 4

Page 118: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 119: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?);

and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 120: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 121: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 ,

F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 122: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 123: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)}

= F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 124: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2

≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 125: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 126: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4.

Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 127: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 128: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4,

α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 129: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.

Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 130: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒

3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 131: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 132: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 (contd..)

Consider

F (b) =b

(b + 1)2.

F ′(b) =1− b

(b + 1)3=⇒ the maximum value of F (b) for b > 0

occurs at b = 1 (Why?); and we find F (1) =1

4.

Hence, if a ≥ 1/4 , F (b) =b

(b + 1)2≤ a for all b > 0 and

α = min{a,F (b)} = F (b) =b

(b + 1)2≤ 1/4, whatever be a.

If a < 1/4 , then certainly α < 1/4. Thus in any case, α ≤ 1/4 .

For b = 1, a ≥ 1/4, α = min{a, 1/4} = 1/4.Thus the best possible α from the theorem gives that the IVP has

a unique solution in |x − 1| ≤ 1/4 =⇒ 3/4 ≤ x ≤ 5/4 .

Santanu Dey Lecture 4

Page 133: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 - Remarks

1 The theorem guarantees existence and uniqueness only in avery small interval!

2 The theorem DOES NOT give the largest interval where thesolution is unique.

3 What is the solution in this case by separation of variables andwhere is it valid? Can you think of extending the solution to alarger interval?

Santanu Dey Lecture 4

Page 134: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 - Remarks

1 The theorem guarantees existence and uniqueness only in avery small interval!

2 The theorem DOES NOT give the largest interval where thesolution is unique.

3 What is the solution in this case by separation of variables andwhere is it valid? Can you think of extending the solution to alarger interval?

Santanu Dey Lecture 4

Page 135: MA 108 - Ordinary Differential Equationsdey/diffeqn_autumn13/lecture4.pdf · Hence the orthogonal trajectories are given by y = kx . Santanu Dey Lecture 4. De nitions 1 Let f be a

Example 2 - Remarks

1 The theorem guarantees existence and uniqueness only in avery small interval!

2 The theorem DOES NOT give the largest interval where thesolution is unique.

3 What is the solution in this case by separation of variables andwhere is it valid? Can you think of extending the solution to alarger interval?

Santanu Dey Lecture 4