10.1 Theory of Linear Systems

INTRODUCTION

Recall that in Section 3.12 we illustrated how to solve systems of n linear differential equations in n unknowns of the form

(1)

where the Pij were polynomials of various degrees in the differential operator D. In this chapter we confine our study to systems of first-order DEs that are special cases of systems that have the normal form

(2)

A system such as (2) of n first-order equations is called a first-order system.

Linear Systems

When each of the functions g1, g2, … , gn in (2) is linear in the dependent variables x1, x2, … , xn , we get the normal form of a first-order system of linear equations:

(3)

We refer to a system of the form given in (3) simply as a linear system. We assume that the coefficients ai j(t) as well as the functions fi(t) are continuous on a common interval I. When fi(t) = 0, i = 1, 2, … , n, the linear system is said to be homogeneous; otherwise it is nonhomogeneous.

Matrix Form of a Linear System

If denote the respective matrices

then the system of linear first-order equations (3) can be written

or simply X′ = AX + F. (4)

If the system is homogeneous, then the matrix form is

X′ = AX. (5)

EXAMPLE 1 Systems Written in Matrix Notation

  1. If X = , then the matrix form of the homogeneous linear system
  2. If X = , then the matrix form of the nonhomogeneous linear system

EXAMPLE 2 Writing a Linear System Without Matrices

Write the linear system

without matrices.

SOLUTION

First, let and so the left-hand side of the given system is

Then, using matrix multiplication and addition, the terms on the right-hand side of the given linear system can be written as a single matrix:

Now two matrices are equal if their entries in the same position are equal. Therefore

An Equation Written as a System

At times it is to your advantage to work with a system of equations rather than with a differential equation. Suppose

(6)

is a linear nth-order differential equation. If we let

(7)

then observe by taking the derivative of each of the terms in (7) we get

Thus a first-order system of n equations is

(8)

EXAMPLE 3 Writing an Equation as a First-Order System

Write the third-order differential equation

as a first-order system of equations using matrix notation.

SOLUTION

First, we write the differential equation as to agree with the form given in (6). Then, using the substitutions we see that

The result is a nonhomogeneous linear system

Using matrices, the foregoing system has the form or

Solution of a Linear System

A solution of a linear system (4) is a set of n differentiable functions defined on a common interval that satisfy each of the differential equations in (3). Equivalently, we have the following definition in terms of matrices.

DEFINITION 10.1.1 Solution Vector

A solution vector on an interval I is any column matrix

whose entries are differentiable functions satisfying the system (4) on the interval.

A solution vector of (4) is equivalent to n scalar equations x1 = Φ1(t), x2 = Φ2(t), … , xn = Φn(t), and can be interpreted geometrically as a set of parametric equations of a space curve. In the cases n = 2 and n = 3, the equations x1 = Φ1(t), x2 = Φ2(t), and x1 = Φ1(t), x2 = Φ2(t), x3 = Φ3(t) represent curves in 2-space and 3-space, respectively. It is common practice to call such a solution curve a trajectory. The plane is also called the phase plane. We will illustrate these concepts in the section that follows, as well as in Chapter 11.

EXAMPLE 4 Verification of Solutions

Verify that on the interval (−∞, ∞)

are solutions of (9)

SOLUTION

From we see that

and .

Much of the theory of systems of n linear first-order differential equations is similar to that of linear nth-order differential equations.

Initial-Value Problem

Let t0 denote a point on an interval I and

where the γi, i = 1, 2, … , n are given constants. Then the problem

(10)

is an initial-value problem on the interval.

THEOREM 10.1.1 Existence of a Unique Solution

Let the entries of the matrices A(t) and F(t) be functions continuous on a common interval I that contains the point t0. Then there exists a unique solution of the initial-value problem (10) on the interval.

Homogeneous Systems

In the next several definitions and theorems we are concerned only with homogeneous systems. Without stating it, we shall always assume that the ai j and the fi are continuous functions of t on some common interval I.

Superposition Principle

The following result is a superposition principle for solutions of linear systems.

THEOREM 10.1.2 Superposition Principle

Let X1, X2, …, Xk be a set of solution vectors of the homogeneous system (5) on an interval I. Then the linear combination

X = c1X1 + c2X2 + … + ckXk,

where the ci, i = 1, 2, …, k are arbitrary constants, is also a solution of the system on the interval.

It follows from Theorem 10.1.2 that a constant multiple of any solution vector of a homogeneous system of linear first-order differential equations is also a solution.

EXAMPLE 5 Using the Superposition Principle

You should practice by verifying that the two vectors

are solutions of the homogeneous system

(11)

By the superposition principle, Theorem 10.1.2, the linear combination

is yet another solution of the system.

Linear Dependence and Linear Independence

We are primarily interested in linearly independent solutions of the homogeneous system (5).

DEFINITION 10.1.2 Linear Dependence/Independence

Let X1, X2, …, Xk be a set of solution vectors of the homogeneous system (5) on an interval I. We say that the set is linearly dependent on the interval if there exist constants c1, c2, …, ck, not all zero, such that

c1X1 + c2X2 + … + ckXk = 0

for every t in the interval. If the set of vectors is not linearly dependent on the interval, it is said to be linearly independent.

The case when k = 2 should be clear; two solution vectors X1 and X2 are linearly dependent if one is a constant multiple of the other, and conversely. For k > 2, a set of solution vectors is linearly dependent if we can express at least one solution vector as a linear combination of the remaining vectors.

Wronskian

As in our earlier consideration of the theory of a single ordinary differential equation, we can introduce the concept of the Wronskian determinant as a test for linear independence. We state the following theorem without proof.

THEOREM 10.1.3 Criterion for Linearly Independent Solutions

Let

be n solution vectors of the homogeneous system (5) on an interval I. Then the set of solution vectors is linearly independent on I if and only if the Wronskian

(12)

for every t in the interval.

It can be shown that if X1, X2, … , Xn are solution vectors of (5), then for every t in I, either W(X1, X2, … , Xn) ≠ 0 or W(X1, X2, … , Xn) = 0. Thus if we can show that W ≠ 0 for some t0 in I, then W ≠ 0 for every t; hence the set of solutions is linearly independent on the interval.

Notice that, unlike our definition of the Wronskian in Section 3.1, here the definition of the determinant (12) does not involve differentiation.

EXAMPLE 6 Linearly Independent Solutions

In Example 4 we saw that and are solutions of system (9).

Clearly X1 and X2 are linearly independent on the interval (−∞, ∞) since neither vector is a constant multiple of the other. In addition, we have

for all real values of t.

DEFINITION 10.1.3 Fundamental Set of Solutions

Any set X1, X2, …, Xn of n linearly independent solution vectors of the homogeneous system (5) on an interval I is said to be a fundamental set of solutions on the interval.

THEOREM 10.1.4 Existence of a Fundamental Set

There exists a fundamental set of solutions for the homogeneous system (5) on an interval I.

The next two theorems are the linear system equivalents of Theorems 3.1.5 and 3.1.6.

THEOREM 10.1.5 General Solution—Homogeneous Systems

Let X1, X2, …, Xn be a fundamental set of solutions of the homogeneous system (5) on an interval I. Then the general solution of the system on the interval is

X = c1X1 + c2X2 + … + cnXn,

where the ci, i = 1, 2, …, n are arbitrary constants.

EXAMPLE 7 General Solution of System (9)

From Example 4 we know that and are linearly independent solutions of (9) on (−∞, ∞). Hence X1 and X2 form a fundamental set of solutions on the interval. The general solution of the homogeneous system on the interval is then

(13)

EXAMPLE 8 General Solution of System (11)

The vectors

are solutions of the system (11) in Example 5 (see Problem 22 in Exercises 10.1). Now

for all real values of t. We conclude that X1, X2, and X3 form a fundamental set of solutions on (−∞, ∞). Thus the general solution of the homogeneous system on the interval is the linear combination X = c1X1 + c2X2 + c3X3; that is,

Nonhomogeneous Systems

For nonhomogeneous systems, a particular solution Xp on an interval I is any vector, free of arbitrary parameters, whose entries are functions that satisfy system (4).

THEOREM 10.1.6 General Solution—Nonhomogeneous Systems

Let Xp be a given solution of the nonhomogeneous system (4) on an interval I, and let

Xc = c1X1 + c2X2 + … + cnXn

denote the general solution on the same interval of the associated homogeneous system (5). Then the general solution of the nonhomogeneous system on the interval is

X = Xc + Xp.

The general solution Xc of the associated homogeneous system (5) is called the complementary function of the nonhomogeneous system (4).

EXAMPLE 9 General Solution—Nonhomogeneous System

The vector Xp = is a particular solution of the nonhomogeneous system

(14)

on the interval (−∞, ∞). (Verify this.) The complementary function of (14) on the same interval, or the general solution of X′ = X, was seen in (13) of Example 7 to be . Hence by Theorem 10.1.6

is the general solution of the nonhomogeneous system (14) on the interval (−∞, ∞).

10.1 Exercises Answers to selected odd-numbered problems begin on page ANS-27.

In Problems 1–8, write the given linear system in matrix form.

  1. = 3x − 5y
    = 4x + 8y
  2. = 4x − 7y
    = 5x
  3. = 5x − 14y + 9t
    = − x + 6y − 2
  4. = −2x + 12y − 3 sin 4t
    = 8x − 3y + 10 cos 4t
  5. = −3x + 4y − 9z
    = 6xy
    = 10x + 4y + 3z
  6. = xy
    = x + 2z
    = −x + z
  7. = xy + z + t − 1
    = 2x + yz − 3t2
    = x + y + z + t2t + 2
  8. = −3x + 4y + et sin 2t
    = 5x + 9z + 4et cos 2t
    = y + 6zet

In Problems 9–12, write the given linear system without the use of matrices.

In Problems 13–16, write the given differential equation as a first-order system using matrix notation.

In Problems 17–22, verify that the vector X is a solution of the given homogeneous linear system.

  1. = 3x − 4y
    = 4x − 7y; X = e−5t
  2. = −2x + 5y
    = −2x + 4y; X = et
  3. X′ = X; X = e−3t/2

In Problems 23–26, the given vectors are solutions of a system X′ = AX. Determine whether the vectors form a fundamental set on the interval (−∞, ∞).


In Problems 27–30, verify that the vector Xp is a particular solution of the given nonhomogeneous linear system.

  1. = x + 4y + 2t − 7
  2. et;

  3. Prove that the general solution of the homogeneous linear system

    on the interval (−∞, ∞) is

    X = c1 et + c2 e−2t + c3 e3t.

  4. Prove that the general solution of the nonhomogeneous linear system

    on the interval (−∞, ∞) is