Docsity
Docsity

Prepare for your exams
Prepare for your exams

Study with the several resources on Docsity


Earn points to download
Earn points to download

Earn points by helping other students or get them with a premium plan


Guidelines and tips
Guidelines and tips

System of ordinary linear differential equations, Lecture notes of Differential Equations

Discusses the system of linear differential equations, in details, taking them in matrix form and performing matrix algebra

Typology: Lecture notes

2024/2025

Uploaded on 04/22/2025

aditya-singh-dvd
aditya-singh-dvd 🇮🇳

1 document

1 / 152

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
Topic 09: Linear System of First Order ODEs
Second Part of MA102 Mathematics II: Winter Semester of AY 2024-2025
MGPP, SN, SHB: IIT Guwahati
Sections 11.1 to 11.7, 7.3, 7.4, 7.6, 7.7
of
S. L. Ross, Differential Equations, 3rd Edition, Wiley
pf3
pf4
pf5
pf8
pf9
pfa
pfd
pfe
pff
pf12
pf13
pf14
pf15
pf16
pf17
pf18
pf19
pf1a
pf1b
pf1c
pf1d
pf1e
pf1f
pf20
pf21
pf22
pf23
pf24
pf25
pf26
pf27
pf28
pf29
pf2a
pf2b
pf2c
pf2d
pf2e
pf2f
pf30
pf31
pf32
pf33
pf34
pf35
pf36
pf37
pf38
pf39
pf3a
pf3b
pf3c
pf3d
pf3e
pf3f
pf40
pf41
pf42
pf43
pf44
pf45
pf46
pf47
pf48
pf49
pf4a
pf4b
pf4c
pf4d
pf4e
pf4f
pf50
pf51
pf52
pf53
pf54
pf55
pf56
pf57
pf58
pf59
pf5a
pf5b
pf5c
pf5d
pf5e
pf5f
pf60
pf61
pf62
pf63
pf64

Partial preview of the text

Download System of ordinary linear differential equations and more Lecture notes Differential Equations in PDF only on Docsity!

Topic 09: Linear System of First Order ODEs

Second Part of MA102 Mathematics II: Winter Semester of AY 2024-

MGPP, SN, SHB: IIT Guwahati

Sections 11.1 to 11.7, 7.3, 7.4, 7.6, 7.

of

S. L. Ross, Differential Equations, 3rd Edition, Wiley

Linear System of First Order ODEs

Text:

I (^) S. L. Ross, Differential Equations, Third Edition, Wiley.

References:

I Lawrence Perko, Differential Equations and Dynamical Systems, Third Edition,

Springer.

I G. F. Simmons & S. G. Krantz, Differential Equations: Theory, Technique, and

Practice, Tata McGraw-Hill.

I Dennis G. Zill, Differential Equations, Cengage Learning, India Edition.

Refer Linear Systems of First Order ODEs:

  1. Ross Book Sections: 11.1, 11.2, 11.3, 11.4, 11.5, 11.6, 11.7, 7.3, 7.4, 7.6, 7.7.
  2. Perko Book Sections: 1.2, 1.3, 1.4, 1.6, 1.7.
  3. Zill Book Sections: 8.1, 8.2, 8.3, 8.4.

System of First Order ODEs

There are many physical problems, more than one element/ object interact with each

other in some manner. To mathematically model such physical problems, we need a

system of two or more differential equations. For example,

I (^) Predator-Prey Model

I Mechanics: Motion of certain Spring-Mass System (Two masses move on

fricrtionless surface)

I Electrical Circuit: Parallel LRC Circuit / more than one loop

I (^) Mixture Problems: Connected Mixing Tanks

Lotka-Volterra Predator-Prey Model

Two different species, say, Foxes and Rabbits interact with in same ecosystem. A

simple model supposes that rabbits eat only grass and foxes eat only rabbits. In other

words, fox is a predator and rabbit is a prey. Let F(t) and R(t) denote the population of

foxes and rabbits respectively, at time t.

If there were no rabbits then foxes won’t have food to eat and hence the population of

foxes would decline in number according to

dF

dt

= −aF where a > 0.

When rabbits are present, the number of interactions/ encounters between these two

species per unit time is proportional to their populations F and R, that is, proportional

to the product FR. Thus when rabbits are present, there is a supply of food to foxes, so

foxes are added to the system at the rate of bFR, b > 0. Therefore

dF

dt

= −aF + bFR where a > 0 and b > 0.

Competition Model

Suppose two different species of animals occupy the same ecosystem, not as predator

and prey, but rather as competitors for the same resources (such as food and living

space) in the system.

In absence of the other, let us assume that the rate at which each population grows is

given by

dx

dt

= ax and

dy

dt

= cy where a > 0 , c > 0.

Since the two species compete, another assumption might be that each of these rates

is diminished simply by the influence or existence of other population. Thus, this model

leads to the following linear system of ODEs. Competition Model

dx

dt

= a x − b y

dy

dt

= c y − d x

where a, b, c and d are positive real constants.

Connected Mixing Tanks

Consider the two tanks A and B as shown in Figure. Let us suppose that tank A

contains 50 gallons of water in which 25 pounds of salt is dissolved. Suppose tank B

contains 50 gallons of pure water. Liquid is pumped into and out of the tanks as

indicated in the Figure. The mixture exchanged between the two tanks and the liquid

pumped out of tank B are assumed to be well stirred. Construct a mathematical model

that describes the number of pounds x 1

(t) and x 2

(t) of salt in tanks A and B,

respectively, at time t.

dx 1

dt

x 1

x 2

dx 2

dt

x 1

x 2

with the initial conditions x 1

(0) = 25 and x 2

Linear System of First Order ODEs

A Linear system of first order ODEs (in normal form) is given by

dx 1

dt

= a 11 (t)x 1 + · · · + a 1 n(t)xn + b 1 (t)

dx 2

dt

= a 21

(t)x 1

  • · · · + a 2 n

(t)x n

  • b 2

(t)

dx n

dt

= a n 1

(t)x 1

  • · · · + a nn

(t)x n

  • b n

(t)

It can be written in the vector differential equation (VDE) form as

dx

dt

= A x + f or

dX

dt

= A X + F or

d

X

dt

A

X +

F ,

A = A(t) =

a 11

(t) · · · a 1 n

(t)

a n 1

(t) · · · a nn

(t)

, x = x(t) =

x 1

(t)

x n

(t)

and f = f(t) =

b 1

(t)

b n

(t)

.

For writing purpose, we prefer the capital letters (instead of bold-face letters) to denote

the Vector Quantities.

So, while writing on paper, one can prefer to use the notation

dX

dt

= A X + F , (1)

where A = A(t) =

a 11

(t) · · · a 1 n

(t)

a n 1

(t) · · · a nn

(t)

,

X = X(t) =

x 1

(t)

x n

(t)

and F = F(t) =

b 1

(t)

b n

(t)

.

Definition: If F ≡ 0 in Equation (1), then the VDE X

′ = AX is called the homogeneous

system. If F. 0 in Equation (1), then the VDE X

′ = AX + F is called the

nonhomogeneous system.

Examples

Example 3: Here y(x) = (y 1

(x), y 2

(x), y 3

(x)). That is, x is independent variable and y 1

,

y 2

, y 3

are dependent variables.

dy 1

dx

= x

2

y 1

  • (x + 1) y 2

  • 3 y 3

  • x

3

dy 2

dx

= xe

x

y 1

  • x

3

y 2

  • 8 y 3

− e

x

dy 3

dx

= x y 1

  • e

x

y 2

  • 5 y 3

  • x

Example 4:

dx

dt

= A x + f ,

where x =

x 1

x 2

x 3

, A =

t

2 (t + 1) 5

2 t

3

e

t

e

−t − 4 cos t

and f =

3 t

3

−e

t

− 8 e

t

.

Solution to the Linear System of First Order ODEs

Definition 1

By a solution of the vector differential equation

dx

dt

= A x + f ,

we mean n × 1 column vector function

Φ(t) =

φ 1

(t)

φ n

(t)

whose components φ 1

, φ 2

,.. ., φ n

each have a continuous derivative on the real

interval a ≤ t ≤ b, which satisfies that

dΦ(t)

dt

= A(t) Φ(t) + f(t) for all t ∈ [a, b].

Homogeneous Linear System of First Order ODEs

A Homogeneous Linear system of first order ODEs is given by

dx 1

dt

= a 11 (t)x 1 + · · · + a 1 n(t)xn

dx 2

dt

= a 21

(t)x 1

  • · · · + a 2 n

(t)x n

dx n

dt

= a n 1

(t)x 1

  • · · · + a nn

(t)x n

It can be written in the vector differential equation (VDE) form as

dx

dt

= A x or

dX

dt

= A X or

d

X

dt

A

X ,

A = A(t) =

a 11

(t) · · · a 1 n

(t)

a n 1

(t) · · · a nn

(t)

and x = x(t) =

x 1

(t)

x n

(t)

.

Example 3

Consider the homogeneous linear VDE x

(t) = A(t) x(t) where

A(t) =

and x(t) =

x 1

(t)

x 2

(t)

x 3

(t)

Then the column vector function

Φ(t) =

e

3 t

− 2 e

3 t

−e

3 t

is a solution of the above given VDE on every real interval a ≤ t ≤ b.

Checking Φ

′ (t) = A(t) Φ(t):

3 e

3 t

− 6 e

3 t

− 3 e

3 t

e

3 t

− 2 e

3 t

−e

3 t

for all t ∈ [a, b].

Outline of Proof for E & U of Solution to the IVP-HLVDE

Step 1:

The solution to the IVP (3) is equivalent to the solution of the vector integral equation

x(t) = x 0

t

t 0

A(s) x(s) ds (4)

which gives x(t 0

) = x 0

.

Step 2: Picard Iterates (For the case t ∈ I with t ≤ t 0

, proof is similar).

Define the Picard iterates as follows:

x 0

(t) = x 0

x n+ 1

(t) = x 0

(t) +

t

t 0

A(s) x n

(s) ds t ≥ t 0

, t ∈ I (5)

for n = 0 , 1 , 2 , 3 ,.. .. Then, the sequence {xn(t)} is well-defined and it is a Cauchy

sequence in R

n for each t. Therefore, the sequence {x n

(t)} converges uniformly on

[a, b] to a function x(t) (say).

Continuation of the Previous Slide

Since x n

(t) → x(t) uniformly on I, we can take the limit under the integral sign of (5) to

get

x(t) = x 0

(t) +

t

t 0

A(s) x(s) ds

which proves that x(t) is the solution of the integral equation (4) and hence x(t) is a

solution to the IVP (3).

Step 3: Uniqueness of the Solution

If x(t) and y(t) are the solutions of (3) then

x(t) − y(t) =

t

t 0

A(s)(x(s) − y(s)) ds =⇒ |x(t) − y(t)| ≤ M

t

t 0

|x(s) − y(s)| ds. Thus for any

given  > 0 , we get from the above inequality, |x(t) − y(t)| <  + M

t

t 0

|x(s) − y(s)| ds. By

Grownwall integral inequality, one can get

|x(t) − y(t)| <  exp(M(t − t 0

)) for t ≥ t 0

Since the above inequality is true for each  > 0 , we can get |x(t) − y(t)| = 0 and hence

x(t) = y(t) for t ≥ t 0

.