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86

a) The eigenvalue method.

Ifλ= 2, thenA−2I=

−2 2 5 −5

. By taking the cross vector we see that we can select the eigenvectorv1= (1,1).

Ifλ=−5, thenA+ 5I= 5 2

5 2

. By taking the cross vector we see that we can select the eigenvectorv2= (−2,5).

The complete solution of the homogeneous system is x=c1e2t

1 1

+c2e−5t −2

5

=

e2t −2e−5t e2t 5e−5t

c1

c2

. It follows that a fundamental matrix is given by

e2t −2e−5t e2t 5e−5t

.

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88

b) Theexponential matrix found by means of Caley-Hamilton’s theorem.

SinceP(λ) =

λ+3 2

2

− 7

2 2

it follows by Cayley-Hamilton’s theorem that

A+3 2I

2

− 7

2 2

I=0, thus B2=

A+3 2I

2

= 7

2 2

I,

where we have putB=A+3 2I.

Now,AandIcommute, so we get by the exponential series that exp(At) = exp

−3 2I+

A+3

2I

t

= exp

−3 2t

exp(Bt)

= exp

−3 2t

n=0

1

(2n)!B2n+ n=0

1

(2n+ 1)!B2n+1

= exp

−3 2t

n=0

1 (2n)!

7 2

2n I+

n=0

1 (2n+ 1)!

7 2

2n B

= exp

−3

2t cosh 7

2t

I+2 7sinh

7 2t

B

=

⎜⎝ 1 2e2t+1

2e−5t 0

0 1

2e2t+1 2e−5t

⎟⎠+1

7(e2t−e−5t)

⎜⎝ 3

2 2

5 −3 2

⎟⎠

=

⎜⎜

⎝ 5 7e2t+2

7e−5t 2 7e2t−2

7e−5t 5

7e2t−5

7e−5t 2 7e2t+5

7e−5t

⎟⎟

⎠,

which is the exponential matrix corresponding to the problem.

2) Sinceet are not of the same type ase2tor e−5t, a reasonable guess is a solution of the form x=

a b

where dx dt =

a b

et.

Then by insertion into the matrix equation, followed by a multiplication by e−t, a

b

=

0 2 5 −3

a b

− 6

0

, dvs.

−1 2 5 −4

a b

= 6

0

. By Cramer’s formulæ or just some fumbling we find

a= 4 and b= 5, and the complete solution is

x(t) = 4

5

et+c1

1 1

e2t+c2

−2 5

e−5t, t∈R, wherec1 andc2 are arbitrary constants.

Alternativelyone may apply the unfortunate solution formula x0(t) =Φ(t)

Φ(t)−1u(t)dt in order to obtain a particular solution.

a) It follows from Φ(t) =

e2t −2e−5t e2t 5e−5t

where detΦ(t) = 7e−3t that

Φ(t)−1=e3t 7

5e−5t 2e−5t

−e2t e2t

=1 7

5e−2t 2e−2t

−e5t e5t

.

b) The integrand is Φ(t)−1u(t) = 1

7

5e−2t 2e−2t

−e5t e5t

−6et 0

= 1 7

−30e−t 6e6t

. c) Then by integrating each coordinate separately,

Φ(t)−1u(t)dt= 1 7

30e−t e6t

. d) A particular solution is

Φ(t)

Φ(t)−1u(t)dt= 1 7

e2t −2e−5t e2t 5e−5t

30e−t e6t

= 1 7

28et 35et

= 4

5

et.

e) The complete solution is x(t) =

4 5

et+

e2t −2e−5t e2t 5e−5t

c1

c2

, t∈R, wherec1 andc2∈Rare arbitrary constants.

90 Example 4.3 Let

A=

a b c d

be any(2×2)matrix, and let

p(λ) = det(A−λI) =λ2−(a+d)λ+(ad−bc) = (λ−λ1)(λ−λ2) be the corresponding characteristic polynomial. Prove that

p(A) := (A−λ1I)(A−λ2I) =0.

When we identify the coefficients of the characteristic polynomial we get λ12=a+d and λ1λ2=ad−bc.

A computation of p(A) gives

p(A) = (A−λ1I)(A−λ2I) =A2−(λ12)A1λ2I

= A2−(a+d)A+ (ad−bc)I=A{A−(a+d)I}+ (ad−bc)I

=

a b c d

a b c d

a+d 0 0 a+d

+ detA·I

=

a b c d

−d b c −a

+ detA·I=A{−detA·A−1}+ detA·I=0, where we have applied the result of Example 4.1.

Example 4.4 LetA be any(2×2) matrix.

1) Prove that

A2= (λ+μ)A−λμI,

whereλandμare the two roots of the characteristic polynomial for A.

Hint: Apply the result of Example 4.3.

2) Conclude from (1) that there exist functionsϕ(t)andψ(t), such that exp(At) =ϕ(t)I+ψ(t)A,

whereϕ(0) = 1andψ(0) = 0.

1) It follows from Example 4.3 that

p(A) = (A−λI)(A−μI) =A2−(λ+μ)A+λμI=0. Then by a rearrangement,

A2= (λ+μ)A−λμI.

2) The exponential matrix is defined by the matrix series exp(At) =I+

n=1

1

n!Antn=I+At+ n=2

1 n!Antn, where the radius of convergence is ∞.

According to (1) every An, n≥2, can be written as a linear combination of Iand A, by using the recursion formula

An=A2An−2= (λ+μ)An−1−λμAn−2, n≥2.

The coefficients only increase as a polynomial, while the denominatorn! is of factorial size. There- fore, this process cannot change the radius of convergence, so we conclude that exp(At) can also be written as a linear combination of IandA, where the coefficients ϕ(t) and ψ(t) are given by power series int of radius of convergence∞,

exp(At) =ϕ(t)I+ψ(t)A. If we here putt= 0, then

exp(A0) =I=ϕ(0)I+ψ(0)A,

and it follows that ϕ(0) = 1 and ψ(0) = 0, because we may assume that I and A are linearly independent. (There is nothing to prove if this is not the case).

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92

Example 4.5 LetA be a(2×2)matrix. We proved in Example 4.4 that A2= (λ+μ)A−λμI,

and

exp(At) =ϕ(t)I+ψ(t)A, ϕ(0) = 1 andψ(0) = 0.

Prove thatϕandψ are the unique solutions of the system of equations

⎧⎨

ϕ(t) =−λμψ(t),

ϕ(t) = (λ+μ)ϕ(t)−λμϕ(t) = 0,

ϕ(0) = 1, ψ(0) = 0. Then find exp(At)explicitly.

Hint: Split the investigation into the to cases (1) λ=μ, and (2)λ=μ. We shall only check the differential equation for exp(At),

d

dtexp(At) = d dt

I+

n=1

1 n!Antn

= n=1

1

(n−1)!Antn−1=Aexp(At). Since

d

dtexp(At) =ϕ(t)I(t)A and

Aexp(At) =ϕ(t)A+ψ(t)A2= (λ+μ)ψ(t)A−ψ(t)λμI+ϕ(t)A, it follows by identification of the coefficients that

ϕ(t) =−λμψ(t),

ψ(t) = (λ+μ)ψ(t)+ϕ(t),

ϕ(0) =−λμψ(0) = 0, ψ(0) = 0 +ϕ(0) = 1. When the latter equation is differentiated, we get

ψ(t) = (λ+μ)ψ(t)+ϕ(t) = (λ+μ)ψ(t)−λμψ(t), hence by a rearrangement,

d2ψ

dt2 −(λ+μ)dψ

dt +λμψ(t) = 0, ψ(0) = 0, ψ(0) = 1, and of course

ϕ(t) =−λμψ(t), ϕ(0) = 1.

The characteristic polynomial for the differential equation ofψis R2−(λ+μ)R+λμ= (R−λ)(R−μ),

with the rootsλandμ.

1) Ifλ=μ, then

ψ(t) =c1eλt+c2eμt where

ψ(0) =c1+c2= 0 and ψ(0) =λc1+μc2= 1, hence c1= 1

λ−μ andc2=− 1

λ−μ, thus ψ(t) = 1

λ−μ(eλt−eμt). We have found that

ϕ(t) =−λμψ(t) = −μ

λ−μ·λeλt+ λ

λ−μ·μeμt, ϕ(0) = 1, so we get by an integration,

ϕ(t) = 1 + t

0

− μ

λ−μλeλτ+ λ λ−μμeμτ

= 1 + λ

λ−μeμt− μ λ−μeλt

λ

λ−μ− μ

λ−μ

= λ

λ−μeμt− μ λ−μeλt. Summing up we have

exp(At) =ϕ(t)I+ψ(t)A= λ

λ−μeμt− μ λ−μeλt

I+ 1

λ−μ(eλt−eμt)A. 2) Ifμ=λ, then

ψ(t) =c1eλt+c2teλt, whereψ(0) =c1= 0, and

ψ(t) =c2eλt+c2λteλt, whereψ(0) =c2= 1. Then

ψ(t) =teλt.

Now,ϕ(t) =−λ2ψ(t) andψ(0) = 1, so ϕ(t) = 1−λ2

t

0 τ eλτdτ = 1−λ"

τ eλτ#t

0+"

eλτ#t

0= 1−λteλt+eλt−1 = (1−λt)eλt. Summing up we get

exp(At) =ϕ(t)I+ψ(t)A= (1−λt)eλtI+teλtA.

94

Example 4.6 Let A be a (2×2) matrix, the characteristic polynomial of which has the root λ of multiplicity 2. Computeexp(At) by using that

exp(At) = exp(λtI+(A−λI)t) =eλtexp((A−λI)t).

When λis a double root, then the characteristic polynomial is (R−λ)2, and it follows from either Cayley-Hamilton’s theorem or Example 4.3 that

(A−λI)2=0. Then

exp((A−λI)t) =I+ (A−λI)t+ n=2

1

n!(A−λI)ntn=I+ (A−λI)t+0= (1−λt)I+tA, and hence

exp(At) =eλtexp((A−λI)t) = (1−λt)eλtI+teλtA, cf. the result of Example 4.5 (2).

Example 4.7 Let A be a (2×2) matrix, the characteristic polynomial of which has the root λ of multiplicity 2. Prove that

Φ(t) =eλtI+teλt(A−λI) is a solution of

dΦ

dt =A Φ(t), Φ(0) =I, and conclude that

exp(At) =eλtI+teλt(A−λI). Since

dΦ

dt =λeλtI+ (1 +λt)eλt(A−λI) =−λ2teλtI+ (1 +λt)eλtA and

A Φ(t) = eλtA+teλt(A−λI)(A−λII) =eλtA+λteλt(A−λI)

= −λ2teλtI+ (1 +λt)eλtA, it follows that

dΦ

dt =A Φ(t). Since

Φ(0) =I+ 0·e0(A−λI) =I,

the initial conditions are also fulfilled. Due to the uniqueness the only solution is exp(At), so exp(At) =eλtI+teλt(A−λI).

Example 4.8 LetA be a(3×3)matrix, the characteristic polynomial of which p(x) = (x−λ)3 has the rootλ of multiplicity 3.

1) Prove thatp(A) := (A−λI)3=0.

2) Let

Φ(t) =eλtI+teλt(A−λI) +1

2t2eλt(A−λI)2. Prove thatΦ(t) = exp(At).

1) This follows immediately form Cayley-Hamilton’s theorem.

96 2) Clearly,Φ(0) =I. Then we just check,

dΦ

dt =λeλtI+(1+λt)eλt(A−λI)+

t+λ

2t2

(A−λI)2 and

A Φ(t) = eλt(A−λII) +teλt(A−λI)(A−λAI) +1

2t2eλt(A−λI)2(A−λII)

= λeλtI+eλt(A−λI) +λteλt(A−λI) +teλt(A−λI)2

2t2eλt(A−λI)2+1

2t2eλt(A−λI)3

= λeλtI+(1+λt)eλt)(A−λI)+

t+λ

2t2

(A−λI)2+0, henceΦ(t) also satisfies the matrix differential equation

dΦ

dt =A Φ(t), Φ(0) =I.

Now, the exponential matrix is the unique solution of this matrix differential equation, so we conclude that

exp(At) =Φ(t) =eλtI+teλt(A−λI)+1

2t2eλt(A−λI)2.

Example 4.9 LetAbe a(3×3)matrix, the characteristic polynomial of whichp(x) = (x−λ)2(x−μ) has a double root λand a simple real rootμ(=λ).

1) Prove that

p(A) := (A−λI)2(A−μI) =0. 2) Prove that

Φ(t) := −eλt

(λ−μ)2(A−λI)(A−μI) + eλt

λ−μ(A−μI) + teλt

λ−μ(A−μI)(A−μI) + eμt

(λ−μ)2(A−λI)2 is a solution of

dΦ

dt =A Φ(t), Φ(0) =I, and then conclude thatΦ(t) = exp(At).

1) This follows immediately from Cayley-Hamilton’s theorem.

2) We get by differentiation, dΦ

dt =

−λ

(λ−μ)2+ 1 λ−μ

eλt(A−λI)(A−μI) + λ

λ−μeλt(A−μI) + λ

λ−μteλt(A−λI)(A−μI) + μ

(λ−μ)2eμt(A−λI)2, which should be compared with

A Φ(t) = − eλt

(λ−μ)2(A−λI)(A−μ)(A−λII) + eλt

λ−μ(A−μI)(A−λII) +teλt

λ−μ(A−λI)(A−μI)(A−λII) + eμt

(λ−μ)2(A−λI)2(A−μII), where we have used that all matrices commute. Now,

(A−λI)2(A−μI) =0, so this expression is reduced to

A Φ(t) = −λ

(λ−μ)2eλt(A−λI)(A−μI) + 1

λ−μeλt(A−λI)(A−μI) + λ

λ−μeλt(A−μI)− λ

λ−μteλt(A−μI)(A−λI) + μ

(λ−μ)2eμt(A−λI)2.

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It follows by the comparison thatΦ(t) satisfies the matrix differential equation dΦ

dt =A Φ(t). Since

Φ(0) = −1

(λ−μ)2(A−λI)(A−μI) + 1

λ−μ(A−μI) + 1

(λ−μ)2(A−λI)2

= 1

(λ−μ)2(A−λI)(μ−λ)I+ 1

λ−μ(A−μI)

= − 1

λ−μ(A−λI) + 1

λ−μ(A−μI) = λ−μ λ−μI=I,

it follows thatΦ(t) fulfils the same initial conditions as exp(At). Since this solution is unique, we conclude that

Φ(t) = exp(At).

Example 4.10 Let A be an (n×n)matrix, the characteristic polynomial p(x) has λ as ann-tuple root.

1) Prove thatp(A) := (A−λI)n=0.

Hint: Apply a coordinate transformationS, such thatA=SΛS−1, whereΛis an upper triangular matrix with only λs in the diagonal.

2) Prove that

exp(At) =eλtexp((A−λI)t) =eλtI+

n−1

j=1

1

j!tjeλt(A−λI)j.

1) By using the hint we get

(A−λI)n = (SΛS−1−λnSIS−1)n=Sn(Λ−λI)nS−n.

Now,Λ−λIis an upper triangular matrix with only zeros in the diagonal. Hence, (Λ−λI)n=0, and the claim is proved.

2) SinceAandIcommute, and

(A−λI)j = (A−λI)n(A−λI)j−n=0 forj≥n, it follows that

exp(At) = exp(λIt+ (A−λI)t) =eλtexp((A−λI)t)

= eλt j=0

1

j!tj(A−λI)j =eλt

n−1

j=0

1

j!tj(A−λI)j.

Example 4.11 Let A be an (n×n) matrix, the characteristic polynomial of which p(x) has the n mutually different eigenvalues λ1,. . .,λn, everyone of multiplicity 1.

1) Prove thatp(A) :=$n

j=1(A−λjI) =0.

2) Letq(x)be the polynomial of degree gradn−1defined by

q(x) = n j=1

⎧⎪

⎪⎩

&n k=jk=1

x−λk

λj−λk

⎫⎪

⎪⎭.

Prove thatq(λj) = 1forj= 1, . . . , n, and conclude thatq(x) = 1 identically.

3) Conclude from (2) that

q(A) :=

n j=1

⎧⎪

⎪⎩

&n k=jk=1

1

λj−λk(A−λkI)

⎫⎪

⎪⎭=I.

4) Prove that

Φ(t) :=

n j=1

⎧⎪

⎪⎩

&n k=jk=1

1

λj−λk(A−λkI)

⎫⎪

⎪⎭eλjt

is a solution of dΦ

dt =A Φ(t), Φ(0) =I, and conclude that

exp(At) = n j=1

⎧⎪

⎪⎩

&n k=jk=1

1

λj−λk(A−λkI)

⎫⎪

⎪⎭eλjt.

1) There exists a coordinate transformationS, such that A=SΛS−1,

whereΛis a diagonal matrix with the diagonal elementsλj and zeros outside the diagonal. Then

p(A) =Sn

⎧⎨

&n j=1

(Λ−λjI)

⎫⎬

S−n=0,

becauseΛ−λjIonly contains elements= 0 in the diagonal, and because thej-th diagonal element is also 0. Sincej goes through{1, . . . , n}, it follows that the product matrix is0.

100 2) When we putx=λj0, then

q(λj0) = n j=1

⎧⎪

⎪⎩

&

k=jk=1

}nλj0−λk

λj−λk

⎫⎪

⎪⎭=

&n k=jk=10

λj0−λk

λj0−λk = 1.

Clearly, the polynomialq(x)−1 has at most degreen−1, and since it hasnzeros,λ1, . . . , λn, we must have q(x)−1 = 0 identically, soq(x) = 1 identically.

3) It follows immediately fromx→Aand 1→Ithat

q(A) = n j=1

⎧⎪

⎪⎩

&n k=jk=1

1

λj−λk(A−λkI)

⎫⎪

⎪⎭=I.

4) Then by (3),

Φ(0) = n j=1

⎧⎪

⎪⎩

&n k=jk=1

1

λj−λk(A−λkI)

⎫⎪

⎪⎭=q(A) =I.

Furthermore, dΦ

dt = n j=1

⎧⎪

⎪⎩

&n k=jk=1

λj

λj−λk(A−λkI)

⎫⎪

⎪⎭eλjt

and

A Φ(t) = n j=1

⎧⎪

⎪⎩

&n k=jk=1

1

λj−λk(A−λjI)

⎫⎪

⎪⎭(A−λjIjI)eλjt

= 0+ n j=1

⎧⎪

⎪⎩

&n k=jk=1

λj

λj−λk(A−λkI)

⎫⎪

⎪⎭eλjt= dΦ dt .

SinceΦ(t) and exp(At) fulfil the same differential equation and same initial conditions, and since the solution is unique, we conclude that

exp(At) =Φ(t) = n j=1

⎧⎪

⎪⎩

&n k=jk=1

1

λj−λk(A−λkI)

⎫⎪

⎪⎭eλjt.

Example 4.12 Computeexp(At)for (1) A=

1 1 0 1

, (2) A=

0 1

−2 3

, (3) A=

0 1

−1 2

.

1) The characteristic polynomial is (λ−1)2, where λ = 1 is a double root. Then it follows from Example 4.7 that

exp(At) =etI+tet(AI) =

et 0 0 et

+

0 tet 0 0

=

et tet 0 et

. 2) The characteristic polynomial is

−λ 1

−2 3−λ

=λ(λ−3)+2 =λ2−3λ+2 = (λ−1)(λ−2).

whereλ= 1 and λ= 2 are simple roots. We get by using the formula of Example 4.11 that exp(At) = 1

1−2(A−2I)et+ 1

2−1(AI)e2t=

2 −1 2 −1

et+

−1 1

−2 2

e2t

=

⎝ 2et−e2t e2t−et 2et−2e2t 2e2t−et

⎠.

102 3) The characteristic polynomial is

−λ 1

−1 2−λ

=λ(λ−2)+1 =λ2−2λ+1 = (λ−1)2,

whereλ= 1 is a double root. Then by Example 4.7, exp(At) =etI+tet(AI) =et

1 0 0 1

+et

−t t

−t t

=

(1−t)et tet

−tet (1+t)et

.

Example 4.13 Computeexp(At)for

(1) A=

⎝1 1 0 0 1 0 0 0 1

⎠, (2) A=

⎝1 1 0 0 1 0 0 0 2

⎠.

1) Clearly,λ= 1 is a root of multiplicity 3, hence by Example 4.8, exp(At) = etI+tet(AI) +1

2t2et(AI)2

= et

⎝1 0 0 0 1 0 0 0 1

⎠+tet

⎝0 t 0 0 0 0 0 0 0

⎠+1 2t2et

⎝0 0 0 0 0 0 0 0 0

=

⎝et tet 0 0 et 0 0 0 et

⎠.

2) Clearly,λ= 1 is a double root, andμ= 2 is a simple root. It then follows from Example 4.9 that exp(At) = − et

(1−2)2(AI)(A−2I) + et

1−2(A−2I) + tet

1−2(AI)(A−2I) + e2t

(1−2)2(AI)2

= −(t+1)et

⎝0 1 0 0 0 0 0 0 1

⎝ −1 1 0 0 −1 0

0 0 0

⎠−et

⎝ −1 1 0 0 −1 0

0 0 0

+e2t

⎝0 1 0 0 0 0 0 0 1

⎝ 0 1 0 0 0 0 0 0 1

=

⎝et tet 0 0 et 0 0 0 e2t

⎠.

Example 4.14 Compute exp(At)for

A=

⎝ 0 1 0

−4 7 −2

−5 7 −1

⎠.

First we find the characteristic polynomial

−λ 1 0

−4 7−λ −2

−5 7 −1−λ

= −λ(λ−7)(λ+1)+10−4(λ+1)−14λ

= −λ3+6λ2+7λ+10−4λ−4−14λ=−λ3+6λ2−11λ+6

= −(λ−1)(λ−2)(λ−3). The eigenvalues areλ= 1, 2, 3. They are all simple.

The equations of the eigenvectors are

⎧⎪

⎪⎪

⎪⎨

⎪⎪

⎪⎪

−λx1+x2 = 0,

−4x1+ (7−λ)x2−2x3 = 0,

−5x1+ 7x2−(λ+ 1)x3 = 0,

dvs.

⎧⎪

⎪⎩

x2=λx1, x3= 7λ−5

λ+ 1 x1. Ifλ= 1, then we can choose the eigenvector (1,1,1).

Ifλ= 2, then we can choose the eigenvector (1,2,3).

Ifλ= 3, then we can choose the eigenvector (1,3,4).

The complete solution of the corresponding system of differential equations is

x=c1et

⎝1 1 1

⎠+c2e2t

⎝1 2 3

⎠+c3e3t

⎝1 3 4

⎠=

⎝et e2t e3t et 2e2t 3e3t et 3e2t 4e3t

⎝c1

c2

c3

⎠.

Hence a fundamental matrix is Φ(t) =

⎝et e2t e3t et 2e2t 3e3t et 3e2t 4e3t

⎠, medΦ(0) =

⎝1 1 1 1 2 3 1 3 4

⎠.

Here,

detΦ(0) =

1 1 1 1 2 3 1 3 4

=

1 0 0 1 1 1 1 2 1

=−1. Then by an inversion of the matrix,

Φ(0)−1=

⎝ 1 1 −1 1 −3 2

−1 2 −1

⎠.

104 Finally, we get

exp(At) = Φ(t)Φ(0)−1=

⎝et e2t e3t et e2t 3e3t et 3e2t 4e3t

⎝ 1 1 −1

1 −3 2

−1 2 −1

=

⎝ et+e2t−e3t et−3e2t+2e3t −et+2e2t−e3t et+2e2t−3e3t et−6e2t+6e3t −et+4e2t−3e3t et+3e2t−4e3t et−9e2t+8e3t −et+6e2t−4e3t

⎠.

Example 4.15 Compute exp(At)for

A=

⎝2 −3 2 2 −5 4 3 −9 7

⎠.

The characteristic polynomial is

1−λ −3 2

2 −5−λ 4

3 −9 7−λ

=

2−λ −3 2

2λ−2 1−λ 0 1 −4 +λ 3−λ

= (λ−1)

2−λ −3 2

2 −1 0

1 −4 +λ 3−λ

= (λ−1){(λ−2)(3−λ) + 4λ−16 + 2−6λ+ 18}

= (λ−1){(λ−2)(3−λ)−2λ+ 4}

= (λ−1)(λ−2)(1−λ) =−(λ−1)2(λ−2). Clearly,λ= 1 is a double root, andμ= 2 is a simple root. Then by Example 4.9,

exp(At) = − eλt

(λ−μ)2(A−λI)(A−μI) + eλt

λ−μ(A−μI) +teλt

λ−μ(A−λI)(A−μI) + eμt

(λ−μ)2(A−λI)2

=−(1+t)et(AI)(A−2I)−et(A−2I) +e2t(AI)2

=−etA(A−2I)−tet(AI)(A−2I)+e2t(AI)2

=−et{(AI)2I}−tet{(AI)2−(AI)}+e2t(AI)2. A small computation gives

(AI)2=

⎝1 −3 2 2 −6 4 3 −9 6

⎝1 −3 2 2 −6 4 3 −9 6

⎠=

⎝1 −3 2 2 −6 4 3 −9 6

⎠=AI.

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