Linear Homogeneous Systems: Theory and Solutions, Study notes of Mathematics

The theory for linear homogeneous systems of differential equations, including the repetition of results from sections 3.2 and 6.1. It covers the trivial solution, theorems 1-3 on constant multiples, sums, and linear combinations of solutions, and the concept of linearly dependent and independent vectors. The document also includes examples and the wronskian determinant.

Typology: Study notes

Pre 2010

Uploaded on 08/18/2009

koofers-user-kx1
koofers-user-kx1 🇺🇸

10 documents

1 / 5

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
6.3 Homogeneous Systems
In this section we give the basic theory for linear homogeneous systems. This “theory” is simply a
repetition results given in Sections 3.2 and 6.1, phrased this time in terms of the system
x0
1=a11(t)x1+a12(t)x2+···+a1n(t)xn(t)
x0
2=a21(t)x1+a22(t)x2+···+a2n(t)xn(t)
.
.
..
.
.
x0
n=an1(t)x1+an2(t)x2+···+ann(t)xn(t)
(H)
or
x0=A(t)x.(H)
Note first that the zero vector z(t)0=
0
0
.
.
.
0
is a solution of (H). As before, this solution
is called the trivial solution. Of course, we are interested in finding nontrivial solutions.
THEOREM 1. If vis a solution of (H) and αis any real number, then u=αvis also a
solution of (H); any constant multiple of a solution of (H) is a solution of (H).
THEOREM 2. If v1and v2are solutions of (H), then u=v1+v2is also a solutions of (H);
the sum of any two solutions of (H) is a solution of (H).
These two theorems can be combined and extended to:
THEOREM 3. If v1,v2,...,vkare solutions of (H), and if c1,c
2,...,c
kare real numbers,
then
c1v1+c2v2+···+ckvk
is a solution of (H); any linear combination of solutions of (H) is also a solution of (H).
DEFINITION 1. Let
v1=
v11(t)
v21(t)
.
.
.
vn1(t)
,v2=
v12(t)
v22(t)
.
.
.
vn2(t)
,..., vk=
v1k(t)
v2k(t)
.
.
.
vnk(t)
be n-component vector functions defined on some interval I. The vectors are linearly dependent on
Iif there exist kreal numbers c1,c
2,...,c
k, not all zero, such that
c1v1(t)+c2v2(t)+···+ckvk(t)0onI.
Otherwise the vectors are linearly independent on I.
244
pf3
pf4
pf5

Partial preview of the text

Download Linear Homogeneous Systems: Theory and Solutions and more Study notes Mathematics in PDF only on Docsity!

6.3 Homogeneous Systems

In this section we give the basic theory for linear homogeneous systems. This “theory” is simply a

repetition results given in Sections 3.2 and 6.1, phrased this time in terms of the system

x

′ 1 =^ a^11 (t)x^1 +^ a^12 (t)x^2 +^ · · ·^ +^ a^1 n(t)xn(t)

x

′ 2 =^ a^21 (t)x^1 +^ a^22 (t)x^2 +^ · · ·^ +^ a^2 n(t)xn(t)

. . .

x ′ n = an 1 (t)x 1 + an 2 (t)x 2 + · · · + ann(t)xn(t)

(H)

or

x

′ = A(t)x. (H)

Note first that the zero vector z(t) ≡ 0 =

is a solution of (H). As before, this solution

is called the trivial solution. Of course, we are interested in finding nontrivial solutions.

THEOREM 1. If v is a solution of (H) and α is any real number, then u = αv is also a

solution of (H); any constant multiple of a solution of (H) is a solution of (H).

THEOREM 2. If v 1 and v 2 are solutions of (H), then u = v 1 + v 2 is also a solutions of (H);

the sum of any two solutions of (H) is a solution of (H).

These two theorems can be combined and extended to:

THEOREM 3. If v 1 , v 2 ,... , vk are solutions of (H), and if c 1 , c 2 ,... , ck are real numbers,

then

c 1 v 1 + c 2 v 2 + · · · + ckvk

is a solution of (H); any linear combination of solutions of (H) is also a solution of (H).

DEFINITION 1. Let

v 1 =

v 11 (t)

v 21 (t)

. . .

vn 1 (t)

, v 2 =

v 12 (t)

v 22 (t)

. . .

vn 2 (t)

,... , vk =

v 1 k(t)

v 2 k(t)

. . .

vnk(t)

be n-component vector functions defined on some interval I. The vectors are linearly dependent on

I if there exist k real numbers c 1 , c 2 ,... , ck, not all zero, such that

c 1 v 1 (t) + c 2 v 2 (t) + · · · + ck vk(t) ≡ 0 on I.

Otherwise the vectors are linearly independent on I.

THEOREM 4. Let v 1 , v 2 ,... , vn be n, n-component vector functions defined on an interval

I. If the vectors are linearly dependent, then

v 11 v 12 · · · v 1 n

v 21 v 22 · · · v 2 n

. . .

vn 1 vn 2 · · · vnn

≡ 0 on I.

The determinant in Theorem 4 is called the Wronskian of the vector functions v 1 , v 2 ,... , vn.

Example 1. The vector functions

u =

t 3

3 t

2

and v =

t − 1

−t

− 2

are solutions of the homogeneous system in Example 3, Section 6.2. Their Wronskian is:

W (x) =

t

3 t

− 1

3 t

2 −t

− 2

= − 4 t.

The vector functions

v 1 =

e

2 t

2 e 2 t

4 e

2 t

,^ v 2 =

e

− 3 t

− 3 e − 3 t

9 e

− 3 t

,^ v 3 =

te

2 t

e 2 t

  • 2te 2 t

4 e

2 t

  • 4te

2 t

are solutions of the homogeneous system

x

x.

Their Wronskian is:

W (x) =

e

2 t e

− 3 t te

2 t

2 e

2 t − 3 e− 3 t e

2 t

  • 2te

2 t

4 e 2 t 9 e − 3 t 4 e 2 t

  • 4te 2 t

= − 25 e

t .

THEOREM 5. Let v 1 , v 2 ,... , vn be n solutions of (H). Exactly one of the following holds:

  1. W (v 1 , v 2 ,... , vn)(t) ≡ 0 on I and the solutions are linearly dependent.
  2. W (v 1 , v 2 ,... , vn)(t) 6 = 0 for all t ∈ I and the solutions are linearly independent.

It is easy to construct sets of n linearly independent solutions of (H). Simply pick any point

a ∈ I and any nonsingular n × n matrix A. Let α 1 be the first column of A, α 2 the second

column of A, and so on. Then let v 1 be the solution of (H) such that v 1 (a) = α 1 , let v 2 be the

solution of (H) such that v 2 (a) = α 2 ,.. ., and let vn be the solution of (H) such that vn = αn.

The existence and uniqueness theorem guarantees the existence of these solutions. Now

W (v 1 , v 2 ,... , vn)(a) = det A 6 = 0.

  1. u =

cos t

sin t

, v =

sin t

cos t

  1. u =

t − t

2

−t

, v =

− 2 t + 4t

2

2 t

  1. u =

te t

t

, v =

e t

  1. u =

2 − t

t

,^ v^ =

t

,^ w^ =

2 + t

t − 2

  1. u =

cos t

sin t

, v =

cos t

sin t

, w =

cos t

sin t

  1. u =

e

t

−e

t

e

t

,^ v^ =

−e

t

2 e

t

−e

t

,^ w^ =

e

t

  1. u =

2 − t

t

, v =

t + 1

, w =

t

t + 2

  1. u =

e t

, v =

, w =

e t

  1. u =

cos (t + π/4)

, v =

cos t)

e t

, w =

sin t)

e t

  1. Given the linear differential system

x

x.

Let

u =

e

2 t

e

2 t

and v =

3 e

3 t

2 e

3 t

(a) Show that u, v are a fundamental set of solutions of the system.

(b) Let V be the corresponding fundamental matrix. Show that

V

′ = AV.

(c) Give the general solution of the system.

(d) Find the solution of the system that satisfies x(0) =

  1. Let V be the matrix function

V (t) =

cos 2t sin 2t

sin 2t − cos 2t

(a) Verify that V is a fundamental matrix for the system

x

x.

(b) Find the solution of the system that satisfies x(0) =

  1. Let V be the matrix function

V (t) =

0 4 te

−t e

−t

1 e

−t 0

(a) Verify that V is a fundamental matrix for the system

x

x.

(b) Find the solution of the system that satisfies x(0) =