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    Math 107 August 6, 2009 (Partial) Solution Manual

    107 (Partial) Solution Manual

    1 Matrices and Determinants

    1.1 Systems of Linear Equations

    2. Solve the system:

    2x +y 2z = 02x y 2z = 0

    x +2y 4z = 0

    2 1 2 02 1 2 01 2 4 0

    rref

    1 0 0 0

    0 1 0 0

    0 0 1 0

    x = 0, y = 0, z = 0

    8. Solve the system:

    x1 +x2 x3 +2x4 = 1x1 +x2 x3 x4 = 1x1 +2x2 +x3 +2x4 = 1

    2x1 +2x2 +x3 +x4 = 2

    1 1 1 2 11 1 1 1 11 2 1 2 12 2 1 1 2

    rref

    1 0 0 0 113

    0 1 0 0 1030 0 1 0 23

    0 0 0 1 23

    x1 =113 , x2 = 103 , x3 = 23 , x4 = 23

    15. Solve the system:

    2x1

    x2

    x3 +x4 +x5 = 0

    x1 x2 +x3 +2x4 3x5 = 03x1 2x2 x3 x4 +2x5 = 0

    2

    1

    1 1 1 0

    1 1 1 2 3 03 2 1 1 2 0

    rref 1 0 0 7

    4 0

    0 1 0 9 5 00 0 1 4 4 0

    x4 and x5 are free variables, while x1 = 7x4 + 4x5, x2 = 9x4 + 5x5, x3 = 4x4 + 4x5

    17. Determine conditions on a, b, and c, so that system is consistent:

    2x y +3z = ax 3y +2z = bx +2y +z = c

    2 1 3 a1 3 2 b1 2 1 c

    2 1 3 a0 52 12 b 12a0 0 0 c + b a

    Thus, c + b a = 0 for the system to be consistent.19. Determine conditions on a, b, c, and d, so that system is consistent:

    1 1 1 1 a1 1 1 1 b1 1 1 1 c

    1 1 1 1 d

    rref

    1 0 0 0 12(a + b)

    0 1 0 0 12(c d)0 0 1 0 12(d b)0 0 0 1 12(c a)

    Thus, there are no conditions on a, b, c, and d for the system to be consistent.

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    Math 107 August 6, 2009 (Partial) Solution Manual

    22. In this case, we have 4 unknowns and 3 equations in a homogeneous linear system. By

    Theorem 1.1, there are infinitely many solutions.

    23. Are there any nontrivial solutions to the system?

    x y +z = 02x +y +2z = 0

    3x 5y +3z = 0 1 1 1 02 1 2 0

    3 5 3 0

    1 1 1 00 3 0 0

    0 0 0 0

    Yes, since in the process of row reduction, we get a row of zeroes.

    26. There are infinitely many answers to each part of this problem. Here are some examples:

    One Solution:x +2y = 1

    x

    y = 0

    No Solution:x +2y +3z = 0

    x +2y 3z = 0x 2y z = 1

    Infinitely Many Solutions:x +2y +3z = 0

    x +2y 3z = 02x +4y z = 0

    28. There are 4 possibilities. With three variables, each equation represents a plane in 3-D space.There are 4 ways that three planes can intersect: (1) No intersection, (2) Intersection at a

    single point, (3) Intersection on a line, and (4) All three planes are identical (intersection

    everywhere on that plane).

    1.2 Matrices and Matrix Operations

    5.

    A 4B =

    7 615 7

    2 17

    9.

    EF =

    0 8 93 5 133 4 10

    2

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    Math 107 August 6, 2009 (Partial) Solution Manual

    11. AE is not a valid multiplication; it is undefined.

    12.

    EA =

    2 0

    3 4

    4 1

    14.

    B(C + D) =

    0 414 816 16

    18. A3 = A A A. A A is not defined, since A is not a square matrix.

    20.

    1

    3 1

    5

    1 1 1 11 1 1 6

    x1

    x2

    x3

    x4

    =

    2

    1

    6

    21.2x1 2x2 +5x3 +7x4 = 124x1 +5x2 11x3 +3x4 = 3

    23. A and B are n n matrices:

    (a) (A + B)2 = (A + B)(A + B) = A(A + B) + B(A + B) = A2 + AB + BA + B2

    (b) In general, AB = BA. This implies that AB + BA = 2AB.

    28. There are many possible answers to this question. Here is one:

    A =

    1 0

    0 0

    , B =

    0 0

    0 1

    , AB =

    0 0

    0 0

    29. (a) A = [ a1 a2 an ], B =

    B1

    B2

    B3

    ...

    Bn

    . Now,

    AB = A

    B1

    B2...

    Bn

    = A

    B1

    0

    0...

    0

    +

    0

    B2

    0...

    0

    + . . . +

    0

    0...

    0

    Bn

    3

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    Math 107 August 6, 2009 (Partial) Solution Manual

    = [ a1 a2 an ]

    B1

    0

    0...

    0

    + [ a1 a2 an ]

    0

    B2

    0...

    0

    + . . . [ a1 a2 an ]

    0

    0...

    0

    Bn

    = AB = a1B1 + a2B2 + . . . + anBn

    (b)

    AB = 2

    12

    4

    +

    1

    1

    1

    + 6

    0

    1

    2

    =

    3

    3

    15

    30. (a) B =

    b1

    b2...

    bn

    , A = [ A1 A2 An ]. Now,

    AB = [ A1 A2 An ]

    b1

    b2...

    bn

    = ([ A1 0 0 ] + [ 0 A2 0 0 ] + . . . + [ 0 0 An ])

    b1

    b2...

    bn

    = [ A1 0 0 ]

    b1

    b2...

    bn

    + [ 0 A2 0 0 ]

    b1

    b2...

    bn

    + . . . + [ 0 0 An ]

    b1

    b2...

    bn

    = AB = b1A1 + b2A2 + . . . + bnAn

    (b)

    AB = 2

    3

    0

    1

    2

    3

    1

    + 3

    15

    2

    =

    1

    12

    7

    4

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    1.3 Inverses of Matrices

    1. Inverse:

    17 27

    37 17

    6. Inverse:

    12 0 12

    111 311 0

    411 111 0

    7. Inverse:

    11

    12

    9

    12

    1

    12 1

    4

    14 14 14 14

    1 12 12 0

    712 14 112 14

    10. Inverse times right hand side:

    11

    12

    9

    12

    1

    12 1

    4

    14 14 14 14

    1 12 12 0

    712 14 112 14

    3

    5

    1

    2

    =

    73

    12

    74

    0

    2912

    x1 =

    7312 , x2 = 74 , x3 = 0, and x4 = 2912 .

    11b. Replace the first row by itself times twice the second row: E =

    1 2

    0 1

    .

    13. Proof of Theorem 1.6: Let E = [eij ] and A = [aij ], so that EA = [n

    k=1

    eikakj ].

    (a) Suppose E switches rows l and m of I. This means that eij = 1 if i equals j and they

    are not equal to l or m or if i = m and j = l or if i = l and j = m. Otherwise eij = 0.

    Consider the ij entry of EA:

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    If i is not equal to l or m, then the only nonzero eik is eii, so

    entij(EA) =n

    k=1

    eikakj = eiiaij = aij .

    Therefore, the ith

    row of EA is the ith

    row of A If i = l, then the only nonzero elk is elm, so

    entlj(EA) =n

    k=1

    elkakj = elmamj = amj .

    Therefore, the lth row of EA is the mth row of A.

    If i = m, then the only nonzero emk is eml, so

    entmj(EA) =n

    k=1

    emkakj = emlalj = alj .

    Therefore, the mth row of EA is the lth row of A, leaving the rest of A the same.

    Thus, EA switches rows l and m of A.

    (b) Suppose E multiplies row l of I by c. Then, ell = c, and eii = 1 for all i = l and eij = 0for i = j. Consider the ij entry of EA:

    If i = l, then the only nonzero eij is eii = 1,

    entij(EA) =n

    k=1

    eikakj = eiiaij = aij .

    Therefore, the ith row of EA is the ith row of A.

    If i = l, then the only nonzero elj is ell = c,

    entlj(EA) =n

    k=1

    elkakj = ellalj = calj .

    Therefore, the lth row of EA is the lth row of A times c.

    Thus, EA multiplies the lth row of A by c, leaving the rest of A the same.

    (c) Suppose E replaces row l by itself plus c times row m. Then, eij = 1 if i = j, elm = c,

    and eij = 0 for i = j for all other i and j. Consider the ij entry of EA: If i = l, then the only nonzero eij is eii = 1,

    entij(EA) =n

    k=1

    eikakj = eiiaij = aij .

    Therefore, the ith row of EA is the ith row of A.

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    17. A + B is not symmetric:

    A + B =

    4 2 21 4 62 6 6

    20. BTB is symmetric for any square matrix B (Theorem 1.14, Part 3). In this case,

    BTB =

    11 2 22 20 102 10 6

    22c. Let A = [aij ] be an n n upper triangular matrix. (The proof for a lower triangular matrixis similar.) () Assume A has all diagonal entries nonzero. This implies that we can do rowoperations on A (multiply row i by 1

    aii) to get an upper triangular matrix with ones on the

    diagonal. These ones can then be use to eliminate everything above in the column using rowoperations (Eliminate off-diagonal aij by replacing row i by row i plus aij times row j, etc.).This leaves the identity. Thus, A is invertible.

    ( = ) (Contrapositive) Assume one of the diagonal entries is zero. If ann = 0, then the lastrow is zero, and the reduced row echelon form for A will have a zero row, and, thus, A will

    not be invertible. Otherwise, let m be the largest m such that amm = 0, i.e. ifi > m, aii = 0.Similar to above, we can do row operations on A (multiply row i by 1

    aii) for all rows below

    row m, to get an upper triangular matrix with ones on the diagonal for all rows beyond row

    m. These ones can then be use to eliminate everything in row m by successively replacing

    row m by row m plus amj times row j for j > m. Since amm = 0, row m will then be a zerorow. Thus, the reduced row echelon form for A will be zero, and A will not be invertible.

    24d. Since A is an symmetric matrix, A = AT. Since A is invertible, it is also true that

    A1 = (AT)1

    By Theorem 1.13, Part(5), for any square matrix, (AT)1 = (A1)T. Thus,

    A1 = A1)T

    Thus, A1 is symmetric.

    26. ( = and ) A and B are row equivalent if and only if there exists elementary matrices,{Ek} such that

    EkEk1 E1A = B

    Let C = EkEk1 E1. By Theorem 1.10, C is the product of elementary matrices if andonly if C is invertible. Thus, C is invertible.

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    32. A3 =

    0 0 0

    0 0 0

    0 0 0

    .

    33. Assume A = [aij ] is an n

    n upper triangulr matrix with zeros along the diagonal. (The

    proof is similar for a lower triangular matrix.) The proof will proceed by induction on the

    number of superdiagonals that are zero, where the kth superdiagonal is define by the entries

    {ai(i+k)} for i = 1 . . . n k, the entries whose columns are k over from the diagonal.

    Base Case k = 1:

    A2 =

    0 a12 a13 a1n0 0 a23 a2n...

    .... . .

    ...

    0 0 0 a(n1)n0 0 0 0

    0 a12 a13 a1n0 0 a23 a2n...

    .... . .

    ...

    0 0 0 a(n1)n0 0 0 0

    =

    0 0 b13 b1n0 0 0 b24 b2n...

    .... . .

    . . ....

    0 0 0 b(n2)n0 0 0 00 0

    0 0

    where bij are some nonzero numbers. Note that every entry 1 column over from the

    diagonal is 0.

    Induction Step. Assume

    Ak =

    0 0 b1(k+1) b1n...

    .... . .

    . . ....

    0 0 0 b(nk)n0

    0 0 0 0

    ......

    . . .. . .

    ...

    0 0 0 0 0

    where every entry in the kth, (k 1)th, . . . , and 1st superdiagonals are zero, i.e every

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    Math 107 August 6, 2009 (Partial) Solution Manual

    of a 1 1 lower triangular matrix is just the single entry. Assume that the determinant of alower triangular n n matrix is the product of the diagonals. Let A be a (n + 1) (n + 1)lower triangular matrix,

    A =

    a11 0 0

    a21 a22 0 0... ... . . . ...an1 an2 ann

    Lets do the cofactor expansion of A about the first row to find the determinant. This gives:

    det(A) =

    a11 0 0a21 a22 0 0

    ......

    . . ....

    an1 an2 ann

    = a11

    a22 0 0a32 a33 0 0

    ......

    . . ....

    an2 an3 ann

    = a11det(B1)

    Now, the matrix B1 is an n n lower triangular matrix, so the determinant of B is theproduct of the diagonals. Thus,

    det(B1) = a22 ann

    and

    det(A) = a11a22 ann

    16. Let A be a square matrix such that row i is c times row j. Let B the matrix obtained from A

    by replacing row i by itself plus c times row j. Thus, row i of B is a zero row. By Corollary1.17, det(B) = 0. By Theorem 1.20, det(B) = det(A). Thus, det(A) = 0.

    If a square matrix has a column that is a scalar multiple of another column, then its deter-

    minant is also zero. In this case, take the transpose of the matrix and apply the just proven

    statement. Then, by Theorem 1.19, the transpose and the original matrix have the same

    determinant.

    1.6 Further Properties of Determinants

    4. The determinant of the matrix is 0. The matrix is not invertible.

    6. A =

    2 31 2

    = det(A) = 1.

    adj(A) =

    2 31 2

    = inv(A) = adj(A)

    det(A)=

    2 31 2

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    10.

    A =

    5 4 12 3 23 1 3

    and det(A) = 24

    A1 =

    2 4 14 3 22 1 3

    and det(A1) = 60

    A2 =

    5 2 1

    2 4 2

    3 2 3

    and det(A2) = 48

    A3 =

    5 4 22

    3 4

    3 1 2

    and det(A3) = 60

    Thus, x = 2.5, y = 2, and z = 2.5.

    13. Suppose E is an elementary matrix.

    (a) If E is obtained from I by multiplying a row of I by a scalar c, then by Theorem 1.20,

    part (2), det(E) = cdet(I) = c.

    (b) If E is obtained from I by replacing a row of I by itself plus c times another row, then

    by Theorem 1.20, part (3), det(E) = det(I) = 1.

    15c. det(A + B) = 28, det(A) = 14, det(B) = 7, det(A) + det(B) = 21. Thus, det(A + B) =det(A) + det(B).

    16 If A and B are square matrices of the same size, then, by Theorem 1.24, det(AB) =

    det(A)det(B) and det(BA) = det(B)det(A). But, determinants of matrices are real num-

    bers, so det(A)det(B) = det(B)det(A). Thus, det(AB) = det(BA).

    1.7 Proofs of Theorems on Determinants

    5. Suppose A is an n n matrix. Consider the ij entry of adj(A)A:

    entij(adj(A)A) =n

    k=1

    Cikakj

    if i = j, then

    entii(adj(A)A) =n

    k=1

    akiCik = det(A)

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    since the sum is the cofactor expansion of A about column i. If i = j, then

    entij(adj(A)A) =n

    k=1

    akjCik

    is the determinant of the matrix, call it B, obtained from A by replacing the jth

    columnof A by the ith column of A. Since this matrix contains two columns with same entries,

    the transpose of B has two identical rows. This implies det(BT) = 0. By Theorem 1.19,

    det(B) = 0. Thus, for i = j,entij(adj(A)A) = 0

    = adj(A)A = det(A)I

    6. Let A =

    A1

    A2

    A3...

    An

    , where Ai is the ith row of A. This implies cA =

    cA1

    cA2

    cA3...

    cAn

    .

    By application of Theorem 1.20 n times,

    det(cA) = cdet

    A1

    cA2

    cA3...

    cAn

    = c2

    det

    A1

    A2

    cA3

    ...

    cAn

    = . . . = cn

    det

    A1

    A2

    ...

    An

    = c

    n

    det(A)

    7. The following lemma will be helpful.

    Lemma 1. If the matrix B is obtained from the matrix A by multiplying one of the columns

    of A by a scalar c, then det(B) = c det(A).

    Suppose B is obtained from A by multiplying one of the columns of A by a c. Note thatBT can be obtained from AT by multiplying a row of AT by c. By Theorem 1.6, part(2),

    det(BT) = c det(AT). By Theorem 1.19, det(AT) = det(A) and det(BT) = det(B). Thus,det(B) = c det(A).

    Let Vn be the n n Vandermonde matrix

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    Thus,

    det(Vn+1) =

    1 1 1 10 x2 x1 x3 x1 xn+1 x10 x22 x21 x23 x21 x2n+1 x21... ... ... ...

    0 xn2 xn1 xn3 xn1 xnn+1 xn1

    =

    x2 x1 x3 x1 xn+1 x1x22 x21 x23 x21 x2n+1 x21

    ..

    .

    ..

    .

    ..

    .xn2 xn1 xn3 xn1 xnn+1 xn1

    By Lemma 1 and the fact that for any positive integer m,

    ym+1 zm+1 = (y z)

    mk=0

    ymkzk

    the determinant becomes

    det(Vn+1) = (x2x1)(x3x1) (xn+1x1)

    1 1 1x2 + x1 x3 + x1

    xn+1 + x1

    ... ... ...n2k=0

    xn2k2 xk1

    n2k=0

    xn2k3 xk1

    n2k=0

    xn2kn+1 xk1

    n1k=0

    xn1k2 xk1

    n1k=0

    xn1k3 xk1

    n1k=0

    xn1kn+1 xk1

    where the second to last row is now explicitly shown. Consider row i of the matrix

    above:

    i1

    k=0

    xi1k2 xk1

    i1

    k=0

    xi1k3 xk1

    i1

    k=0

    xi1kn+1 xk1

    If we multiply row i by x1, it becomes

    ik=1

    xik2 xk1

    i1k=1

    xik3 xk1

    n1k=1

    xikn+1xk1

    Thus, adding x1 times row i to row i + 1,i

    k=0

    xik2 xk1

    ik=1

    xik2 xk1

    ik=0

    xik3 xk1

    i1k=1

    xik3 xk1

    ik=0

    xikn+1xk1

    n1k=1

    xikn+1xk1

    = xi2 xi3 xin+1 By Theorem 1.20, adding a multiple of one row to another does not change the deter-

    minant, so if for each i we add x1 times row i to row i + 1, we obtain

    det(Vn+1) = (x2 x1)(x3 x1) (xn+1 x1)

    1 1 1x2 x3 xn+1...

    ......

    xn22 xn23 xn2n+1

    xn12 xn13 xn1n+1

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    2. (b) Not a subspace since it is not closed under scalar multiplication:

    c

    y + z + 1

    y

    z

    =

    cy + cz + c

    cy

    cz

    ,

    which is not in the subset if c = 1.(d) Not a subspace since it is not closed under scalar multiplication:

    c

    x

    y

    x2 + y2

    =

    cx

    cy

    cx2 + cy2

    ,

    which is not in the subset for all c.

    3. (a) Subspace

    (b) Not a subspace (not closed under both addition and scalar multiplication)(c) Subspace

    (d) Subspace

    (e) Not a subspace (not closed under both addition and scalar multiplication)

    5. The solutions to that linear system do not define subspace. The set of solutions is not closed

    under addition or scalar multiplication: Let X1 and X2 be two solutions to AX = B, with B

    nonzero. Then,

    A(X1 + X2) = AX1 + AX2 = B + B = 2B

    = B

    A(cX1) = cAX1 = cB = B, if c = 1

    11. Consider 1 2

    1 3

    c1

    c2

    =

    x1

    x2

    Since

    1 21 3 = 5 = 0, given x1 and x2, this system has a unique solution for c1 and c2.

    Thus, it spans R2. Since the solution c1 = c2 = 0 is unique for x1 = 0 and x2 = 0, the vectors

    are also linearly independent. Thus, they are a basis for R2.

    12. Consider 1 5

    2 4

    c1

    c2

    =

    x1

    x2

    Since

    1 52 4 = 6 = 0, given x1 and x2, this system has a unique solution for c1 and c2.

    Thus, it spans R2. Since the solution c1 = c2 = 0 is unique for x1 = 0 and x2 = 0, the vectors

    are also linearly independent. Thus, they are a basis for R2.

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    The matrix has determinant 1, so the system has a unique solution, c1 = c2 = c3 = c4 = 0.

    Thus, the vectors are linearly independent.

    14. Assume c1

    2

    10

    + c2

    1

    3

    1

    + c3

    1

    41

    = 0. Since

    det(A) =

    2 1 1

    1 3 41 3 4

    = 14 = 0

    there is a unique solution to the coefficient problem, A

    c1

    c2

    c3

    = b. If b = 0, then since the

    solution is unique,

    c1c2c3

    = 0, so the vectors are linearly independent. For any other b, asolution exists, so the vectors span R3. Therefore, the vectors form a basis.

    17. Assume c1(x2 + x + 1) + c2(x

    2 x + 1) + c3(x2 1) = 0. Then,

    1 1 1

    1 1 01 1 1

    c1

    c2

    c3

    = 0

    The matrix has determinant equal to 4, so the system has a unique solution c1 = c2 = c3 = 0.

    Thus, the vectors are linearly independent. The nonzero determinant also implies a unique

    solution to the nonhomogeneous problem, which implies that the vectors span P2. Thus, the

    vectors are a basis.

    21. Consider c1(x + 1) + c2(x + 2) + c3(x + 3) = 0 or the equivalent system

    1 1 1

    1 2 3

    c1

    c2

    c3

    = 0

    Apply row operations, the matrix above becomes1 0 10 1 2

    Thus, c1 = c3, and c2 = 2c3 with c3 a free variable are solutions. For example, c1 = 1,c2 = 2, c3 = 1 is a solution. Thus, the vectors are not linearly independent and, therefore,not a basis.

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    4. (c) c1

    0 1

    0 1

    + c2

    1 0

    0 1

    + c3

    1 0

    0 0

    + c4

    0 1

    1 0

    = 0 implies

    c2 + c3 = 0

    c1

    + c4

    = 0

    c4 = 0

    c1 + c2 = 0

    = c1 = 0 = c2 = 0 = c3 = 0. Thus, the vector matrices are linearlyindependent. Since there are 4 of them, they form a basis for M22(R).

    (d) There are 5 vector matrices in the set and dim(M22(R)) = 4, so the set cannot be a

    basis.

    7. 1 1 1

    1 1 01 1 2

    rref

    1 1 00 0 1

    0 0 0

    Thus, x2 is a free variable and x1 x2 = 0, x3 = 0. Thus, every vector in the nullspace is

    of the form:

    x2

    x2

    0

    . Thus, a basis for the nullspace is {

    1

    1

    0

    }. A basis for the rowspace is

    {[1 -1 0], [0 0 1]}.

    1

    1 1

    1 1 01 1 2

    rcef 1 0 0

    0 1 0

    2 1 0

    So, a basis for the column space is {

    1

    0

    2

    ,

    0

    1

    1

    }. Thus, the rank of the matrix is 2.

    10. 2 1 3 41 0

    1 3

    rref

    1 0 1 30 1

    5 2

    Thus, x3 and x4 are free variables and x1 x3 + 3x4 = 0, x2 5x3 + 2x4 = 0. Therefore, anyvector in the nullspace can be written

    x3

    5x3

    x3

    0

    +

    3x42x4

    0

    x4

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    Therefore, a basis for the nullspace is {

    1

    5

    1

    0

    ,

    320

    1

    }. A basis for the rowspace is {[1 0 -1 3],

    [0 1 -5 2]}. 2 1 3 41 0 1 3

    rref

    1 0 0 0

    0 1 0 0

    So, a basis for the column space is {

    1

    0

    ,

    0

    1

    }. Thus, the rank of the matrix is 2.

    14.

    0 1 2 4

    2 1 0 2

    1 0 1 1

    rref

    1 0 1 00 1 2 0

    0 0 0 1

    So, the rank of the matrix is 3. Thus, the dimension of the subspace spanned by the vectors

    is 3, so it is all ofR3. So, a basis for the subspace is {

    1

    0

    0

    ,

    0

    1

    0

    ,

    0

    0

    1

    }

    18. Suppose A is an m n matrix, with m > n. Let B be the reduced row echelon form forA. Then, the RS(A) = RS(B) by Theorem 2.13, since A and B are row equivalent. Also,

    since m > n, B has at most n nonzero rows and since B is in reduced row echelon form, the

    nonzero rows of B form a basis for RS(B), and thus, RS(A). Therefore, the set of rows of

    A is subset of RS(A) with more vectors in it than the basis. Thus, by Lemma 2.8, the set of

    rows is linearly dependent.

    2.5 Wronskians

    5. w(x2

    1, x2 + 1, x + 1) =

    x2 1 x2 + 1 x + 12x 2x 1

    2 2 0

    = 4

    = 0 for some x, so the functions are

    linearly independent.

    6. w(ex, e2x, e3x) =

    ex e2x e3x

    ex 2e2x 3e3x

    ex 4e2x 9e3x

    = 2e6x = 0 for some x, so the functions are linearly

    independent.

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    12. By trigonometric identity, for all x,

    cos(2x) = cos2(x) sin2(x)

    Thus, for all x,

    cos(2x) cos2

    (x) + sin2

    (x) = 0

    Therefore, the functions are linearly dependent.

    14. (a) No, since one (or all) of the functions could be zero on the interval (c, d), and linearly

    dependent there, but be, for example, x, x2, x3,. . . , etc. on the rest of the interval and

    stil be linearly independent on (a, b).

    (b) Yes, since if there are no scalars to make a linear combination of the functions equal to

    zero on all of (c, d), there cannot be scalars to make a linear combination of the functions

    equal to zero on all of any interval (a, b) that includes (c, d).

    3 First Order Ordinary Differential Equations

    4 Linear Differential Equations

    4.1 The Theory of Higher Order Linear Differential Equations

    2. 2nd order, linear

    3. 4th order, linear

    6. (1, )

    10. The two functions solve the ODE:

    1x

    : x :

    x2( 2x3

    ) + x( 1x2

    ) 1x

    = 0 x2(0) + x(1) x = 0

    The two functions are linearly independent since

    1x

    x

    1x2

    1

    = 2x , which is nonzero every-where. Thus, they are a fundamental set of solutions and the general solution is given by

    c11

    x+ c2x

    Solving using the initial conditions, y(1) = 0, y(1) = 1,

    c1 + c2 = 0

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    c1 + c2 = 1

    gives, c1 = 12 , c2 = 12 , which gives the solution 12x + 12x.

    11. The three functions solve the ODE:

    ex : e2x : e3x :

    ex 7ex + 6ex = 0 8e2x 7(2e2x) + 6e2x = 0 27e3x 7(3e3x) + 6e3x = 0

    The Wronskian of the three functions is

    ex e2x e3x

    ex 2e2x 3e3xex 4e2x 9e3x

    = 20

    so the functions are linearly independent. The general solution to the ODE is

    c1ex + c2e

    2x + c3e3x

    Using the initial condition, y(0) = 1, y(0) = 0, y(0) = 0 gives

    c1 + c2 + c3 = 1, c1 + 2c2 3c3 = 0, c1 + 4c2 + 9c3 = 0

    which has solution c1 =32 , c2 = 35 , and c3 = 110 , giving the solution to the ODE as

    3

    2ex

    3

    5e2x +

    1

    10e3x

    15. The general solution is given by

    ex + c1ex + c2e2x + c3e3x

    For the initial conditions, y(0) = 1, y(0) = 0, y(0) = 0, this gives

    1 + c1 + c2 + c3 = 1, 1 + c1 + 2c2 3c3 = 0, 1 + c1 + 4c2 + 9c3 = 0

    which has solution c1 = 0, c2 =1

    5

    , c3 =

    1

    5

    , giving the solution to the ODE as

    ex +1

    5e2x 1

    5e3x

    17. {x, x2} is a fundamental set of solutions:

    x : x2 :

    12x

    2(0) x(1) + x = 0 12x2(2) x(2x) + x2 = 0

    25

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    (b) The initial conditions imply that c1 c2 + c3e5 = 1, c2 + 5c3e5 = 0, and 25c3e5 = 2.Thus, c1 =

    1325 , c2 =

    25 , c3 =

    2e5

    25 so the solution to the IVP is

    13

    25 2

    5x +

    2

    25e5(x+1)

    23. (a) The characteristic polynomial has roots 0, 2, and 3, the general solution is

    c1 + c2e2x + c3e3x

    (b) The initial conditions imply that c1 + c2 + c3 = 1, 2c2 + 3c3 = 0, and 4c2 + 9c3 = 2.Thus, c1 =

    23 , c2 =

    15 , c3 =

    215 so the solution to the IVP is

    2

    3+

    1

    5e2x +

    2

    15e3x

    24. The hard way.

    (a) The characteristic polynomial has roots 0 and 2 i, the general solution is

    c1 + c2e2x sin x + c3e

    2x cos x

    (b) The initial conditions imply that c1+c2e2 sin(1)+c3e

    2 cos(1) = 1, e2(2 sin(1)+cos(1))c2+

    e2(2 cos(1) sin(1)c3 = 0, and e2(3 sin(1) + 4 cos(1))c2 + e2(4 sin(1) + 3 cos(1))c3 = 2.Thus, c1 =

    75 , c2 = e

    2(45 cos(1) 25 sin(1)), c3 = e2(25 cos(1)+ 45 sin(1)), so the solutionto the IVP is

    7

    5+ e2(

    4

    5cos(1) 2

    5sin(1))e2x sin(x) + e2(2

    5cos(1) +

    4

    5sin(1))e2x cos(x)

    24. The easy way.

    (a) The characteristic polynomial has roots 0 and 2 i, the general solution is

    c1 + c2e2x2 sin(x 1) + c3e2x2 cos(x 1)

    (b) The initial conditions imply that c1 + c3 = 1, c2 + 2c3 = 0, and 4c2 + 3c3 = 2. Thus,

    c1 =75 , c2 =

    45 , c3 =

    25 , so the solution to the IVP is

    7

    5+

    4

    5e2x2 sin(x 1) 2

    5e2x2 cos(x 1)

    The two solutions can be seen to be identical by the fact that

    sin(AB) = sin(A) cos(B) cos(A)sin(B) and cos(AB) = cos(A)cos(B) sin(A) sin(B)

    29. The general solution is c1e2x + c2e3x + c3xe3x + c4e3x + c5xe3x.

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    30. The general solution is

    c1 + c2x + c3x2 + c4e

    4x + c5xe4x+

    exc6 cos(

    2

    2x) + c7 sin(

    2

    2x) + c8x cos(

    2

    2x) + c9x sin(

    2

    2x)+

    e1

    2x

    c10 cos(

    3

    2x) + c11 sin(

    3

    2x)

    40. The conditions on the roots r1, . . . , rn real and distinct, so that the equation decays to 0 as

    x are that ri < 0 for all i.

    41. The conditions on the roots r1, . . . , rn real, but not necessarily distinct, so that the equation

    decays to 0 as x are that ri < 0 for all i.

    42. The conditions on the roots r1, . . . , rn possibly complex, so that the equation decays to 0 as

    x are that Re(ri) < 0 (the real part is negative) for all i.

    4.3 The Method of Undetermined Coefficients

    1. The characteristic polynomial of the homogeneous equation has roots 3 and 2, so a fun-damental set for the homogeneous equation is e3x, e2x. Trying a particular solution of the

    form Ae2x yields

    4Ae2x 2Ae2x 6Ae2x = 3e2x

    or A = 34 . Thus, the general solution is

    34

    e2x + c1e3x + c2e

    2x

    4. The characteristic polynomial of the homogeneous equation has roots 1 and 12 , so a fun-damental set for the homogeneous equation is ex, e

    1

    2x. Trying a particular solution of the

    form A cos(x) + B sin(x) yields

    2A cos(x) 2B sin(x) 3A sin(x) + 3B cos(x) + A cos(x) + B sin(x) = cos(x)

    or A + 3B = 1 and B 3A = 0, which has solution A = 110 , B = 310 . Thus, the generalsolution is

    110

    cos(x) +3

    10sin(x) + c1e

    x + c2e1

    2x

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    9. The characteristic polynomial of the homogeneous equation has roots 2i, so a fundamentalset for the homogeneous equation is cos(2x), sin(2x). Trying a particular solution of the form

    Ax cos(2x) + Bx sin(2x) yields

    16A sin(2x)+16B cos(2x)

    16Ax cos(2x)

    16Bx sin(2x)+16Ax cos(2x)+16Bx sin(2x) = 3cos(2x)

    or 16A = 0 and 16B = 3, which has solution A = 0, B = 316 . Thus, the general solution is3

    16x sin(2x) + c1 cos(2x) + c2 sin(2x)

    11. The characteristic polynomial of the homogeneous equation has roots 0 and 8, so a funda-mental set for the homogeneous equation is 1, e8x. Trying a particular solution of the form

    Ax3 + Bx2 + Cx yields

    6Ax + 2B + 24Ax2

    + 16Bx + 8C = 2x2

    7x + 3or 24A = 2, 6A + 16B = 7 and 2B + 8C = 3, which has solution A = 112 , B = 1532 , C = 63128 .Thus, the general solution is

    1

    12x3 15

    32x2 +

    63

    128x + c1 + c2e

    8x

    14. The characteristic polynomial of the homogeneous equation has roots 2 and 4, so a fun-damental set for the homogeneous equation is e2x, e4x. Trying particular solutions of the

    forms Ax2 + Bx + C, Dxe2x and F cos(4x) + G sin(4x) yields

    6A + 12Ax + 6B 24Ax2 24Bx 24C = 3x2

    12Dxe2x + 12De2x + 6De2x + 12Dxe2x 24Dxe2x = 5e2x

    48F cos(4x)48G sin(4x)24F sin(4x)+24G cos(4x)24F cos(4x)24G sin(4x) = 6 sin(4x)

    or 24A = 3, 12A24B = 0, 6A+6B24C = 0, 18D = 5, 72F+24G = 0, 72G24F =6, which has solution A = 18 , B = 116 , C = 364 , D = 518 , F = 140 , G = 340 . Thus, thegeneral solution is

    18

    x2 116

    x 364

    518

    xe2x +1

    40cos(4x) +

    3

    40sin(4x) + c1e

    2x + c2e4x

    18. The characteristic polynomial of the homogeneous equation has a double root 2, so a fun-damental set for the homogeneous equation is e2x, xe2x. Trying particular solutions of the

    forms Ax + B and Ccos(3x) + D sin(3x) yields

    4A + 4Ax + 4B = 2x

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    So,

    yp(x) =1

    2

    3x2ex 6xex 5ex ex 12

    3x2ex 6xex + 5ex ex

    = 3

    2 x2

    3x 5

    2 3

    2 x2

    + 3x 5

    2 = 3x2

    5

    2. The roots of the characteristic polynomial are 3 and 2, making e3x and e2x a fundamentalset of solutions to the homogeneous equation. w(e3x, e2x) = 5ex, so, then, yp = u1(x)e3x +u2(x)e

    2x, with

    u1(x) =

    e2x4ex

    5ex = 4

    10e2x

    and

    u2(x) =e3x4ex5ex = 415 e3x

    so,

    yp(x) = 410

    e2xe3x 415

    e3xe2x

    = 23

    ex

    So, the general solution is

    y = 2

    3 ex

    + c1e3x

    + c2e2x

    3. The characteristic polynomial has a double root at 3, so a fundamental set of solutions ise3x, xe3x. Thus, w(e3x, xe3x) = e6x. Then, if yp(x) = u1(x)e3x + u2(x)xe3x,

    u1(x) =

    3e3xxe3x

    e6x= 1

    2xe6x +

    1

    12e6x

    and

    u2(x) =

    3e3xe3x

    e6x=

    1

    2e6x

    Thus,

    yp(x) = (12

    xe6x +1

    12e6x)e3x +

    1

    2e6xxe3x

    =1

    12e3x

    So, the general solution is

    y =1

    12e3x + c1e

    3x + c2xe3x

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    5 Linear Transformations and Eigenvalues and Eigenvectors

    5.1 Linear Transformations

    3. Not a linear transformation: T(x1 + x2, y1 + y2, z1 + z2) = T(x1, y1, z1) + T(x2, y2, z2).4. Linear transformation

    7. Linear transformation

    12. Not a linear transformation: T(A + B) = det(A + B) = det(A) + det(B) = T(A) + T(B).

    18.

    1 1 3 12 3

    1

    2

    3 7 5 3

    20. Let

    A =

    1 1 0

    1 0 10 1 1

    Then,

    A1 =

    1 1 10 1 1

    1 0 1

    (a) A1

    2

    1

    4

    =

    5

    36

    . So, T

    2

    1

    4

    = 5T

    1

    1

    0

    3T

    10

    1

    + 6T

    0

    1

    1

    or

    T

    2

    1

    4

    =

    5

    0

    50

    +

    630

    0

    +

    6

    0

    0

    6

    =

    5

    35

    6

    (b) A1

    x

    y

    z

    =

    x y zy + z

    x z

    . So,

    T

    x

    y

    z

    = (x y z)T

    1

    1

    0

    + (y + z)T

    10

    1

    + (x z)T

    0

    1

    1

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    or

    T

    x

    y

    z

    =

    x y z0

    x + y + z

    0

    +

    2y + 2z

    y + z

    0

    0

    +

    x z0

    0

    x

    +z

    =

    2x + y

    y + z

    x + y + z

    x

    +z

    33. Suppose

    x

    y

    =

    r cos

    r sin

    . Then,

    T

    x

    y

    =

    r cos( + )

    r sin( + )

    =

    r cos cos r sin sin r sin cos + r cos sin

    =

    x cos y sin y cos + x sin

    =

    cos sin sin cos

    xy

    35. For any linear transformation, T : V V, either dim(ker(T)) = 0 or dim(ker(T)) > 0, butnot both can be true. The second inequality is 2. We show that dim(ker(T)) = 0 implies 1.

    Let v1, . . . , vn be a basis of the n-dimensional vector space V. Then, T(v1), . . . , T(vn) are a

    set of n vectors in V. Assume there are scalars {ci} so that

    c1T(v1) + c2T(v2) + . . . + cnT(vn) = 0

    Then,

    T(c1v1 + c2v2 + . . . + cnvn) = 0

    Since dim(ker(T)) = 0, this implies that c1v1 + . . . + cnvn = 0, and consquently, that c1 =

    c2 = = cn = 0, since v1, . . . , vn is a basis. Thus, T(v1), . . . , T(vn) are linearly independentvectors in V. Since there are n of them, they also form a basis for V. Thus, they also span

    V. Therefore, for any vector v V, there exist {ai} so that

    v = a1T(v1) + a2T(v2) + . . . + anT(vn) = T(a1v1 + . . . + anvn)

    Defining u = a1v1 + . . . + anvn, gives T(u) = v and statement 1.

    36. If T : V W is 1-1, then T(x1) = T(x2) = x1 = x2. Suppose u ker(T). Then,T(u) = T(0) = u = 0. So, the kernel is only the zero vector.Ifker(T) is only the zero vector, suppose T(x1) = T(x2) for x1, x2 V. Then, T(x1x2) = 0,which implies x1x2 ker(T). But, zero is the only vector in the kernel ofT, so x1x2 = 0,or x1 = x2. So, T is 1-1.

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    5.2 The Algebra of Linear Transformations

    5. ST

    x

    y

    = S

    x + 3y

    x y

    =

    x + 7y

    3x + y

    6. T S

    xy

    = T

    2x yx + 2y

    =

    5x + 5yx 3y

    8. T S(ax + b) = T(ax 2a + b) = ax + 2a 2a + b = ax + b

    11. Basis={e3x, ex}

    14. Basis={sin x, cos x, x sin x, x cos x}

    17. Let f(x), h(x) C. Then,

    Tg(x)(f + h) = g(x)(f(x) + h(x)) = g(x)f(x) + g(x)h(x) = Tg(x)(f) + Tg(x)(h)

    and

    Tg(x)(cf) = g(x)(cf(x)) = cg(x)f(x) = cTg(x)

    So, Tg(x) is a linear transformation.

    20. (a) Ifu ker(T), then T(u) = 0. T(u + v) = T(u) + T(v) = T(v).(b) If T(u) = T(v), then T(u) T(v) = 0 = T(u v) = 0, so that u v ker(T).

    23. (a) A =1 3

    1 1

    , B =2 11 2

    (b) C =

    1 7

    3 1

    , BA =

    2 11 2

    1 3

    1 1

    =

    1 7

    3 1

    5.3 Matrices for Linear Transformations

    1. (a) [T] =

    1 1

    1 1

    (b) The change of basis from to is given by P = 1 21 1 .

    (c) The change of basis from to is given by P1 =

    1 21 1

    .

    (d) [T] = P1[T]P =

    4 72 4

    .

    4. (Assuming a spurious x2 in the fourth row.)

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    (b) The change of basis from to is given by P =

    1 1

    1 1

    .

    (c) The change of basis from to is given by P1 =

    12

    12

    12 12

    .

    (d) [T] = P1[T]P =

    0 1

    1 0

    .

    (e) [v] =

    23

    . [v] = P

    1[v] =

    1252

    .

    (f) [T(v)] = [T][v] =

    52

    12

    .

    (g) T(v) = 52(sin(x) + cos(x)) 12(sin(x) cos(x)) = 2 sin(x) + 3 cos(x).

    9. (a) [T] =

    1 0

    1

    1 1 00 1 1

    (b) [T(v)] = [T]

    [v] =

    1 0 1

    1 1 00 1 1

    1

    23

    =

    235

    (c) T(v) = 2v1 3v2 + 5v3.

    5.4 Eigenvalues and Eigenvectors

    5. The eigenvalues are 2

    3 and 23, with basis eigenvectors

    32

    1

    and

    32

    1

    , respectively.

    8. The eigenvalues are 2 and 1, with basis eigenvectors

    111

    for 2 and

    1

    0

    0

    for 1.

    9. The eigenvalue is 4 with basis eigenvector

    0

    01

    .

    16. The eigenvalues are 2i and 2i with basis eigenvectors

    1 2i1

    and

    1 + 2i

    1

    , respectively.

    17. The eigenvalues are 1, i, and i with basis eigenvectors

    1

    0

    0

    ,

    0

    1

    i

    , and

    0

    1

    i

    , respectively.

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    20. IfD is diagonal matrix, the eigenvalues of D are the diagonal entries of D. The bases for the

    eigenspaces are just the standard basis vectors for Rn.

    26. If A is a square matrix, then eigenvalues of A are the so that det(I A) = 0. Sincedet(B) = det(BT) for any square matrix B, det(I

    A) = det (I A)

    T = det(I AT).

    Thus, det(I A) = 0 if and only if det(I AT), so A and AT have the same eigenvalues.

    5.5 Similar Matrices, Diagonalization, and Jordan Form

    5. A is diagonalizable:

    D =

    12 0

    0 12

    , P =

    12

    3 12

    3

    1 1

    8. A is not diagonalizable, not enough eigenvectors.

    9. A is not diagonalizable, not enough eigenvectors.

    16. A is diagonalizable:

    D =

    2i 0

    0 2i

    , P =

    1 2i 1 + 2i

    1 1

    17. A is diagonalizable:

    D =

    1 0 0

    0 2i 0

    0 0

    2i

    , P =

    1 0 0

    0 1 1

    0 i

    i

    31. Suppose A and B are similar matrices. Then, A = P1BP for some invertible matrix P.

    Thus, A I = P1BP I for any scalar . Therefore,

    det(A I) = det(P1BP I)= det

    P1(BP P I) = det P1(B PIP1)P

    = det(P1)det(B I)det(P)= det(B I)

    Thus, A and B have the same characteristic polynomial.

    36. Let A be a n n matrix with n distinct eigenvalues. Since the bases of eigenspaces corre-sponding to different eigenvalues are linearly independent and A has n eigenspaces, there are

    n linearly independent eigenvectors of A. Thus, A is diagonalizable by Theorem 5.18.

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    6 Systems of Linear Differential Equations

    6.1 The Theory of Systems of Linear Differential Equations

    1. Y = 2c1e

    2x + 3c2e3x

    4c1e2x

    + 3c2e3x

    4 12 1

    Y =

    4c1e

    2x + 4c2e3x 2c1e2x c2e3x

    2c1e2x + 2c2e

    3x + 2c1e3x + c2e

    3x

    = Y

    4. W(

    e2x

    0

    0

    ,

    0

    3 cos(5x)

    3 sin(5x)

    ,

    0

    sin5x

    cos5x

    ) = e2x(3 cos2(5x) + 3 sin2(5x)) = 3e2x = 0 for all x.

    Therefore, the functions are linearly independent on the whole interval (, ).

    5. The general solution to the problem is c1ex

    c2e2x

    . A matrix of fundamental solutions isex 0

    0 e2x

    .

    9. Y(0) =

    2

    1

    gives the specific solution

    2ex

    e2x

    .

    17. Being a matrix, M, of fundamental solutions implies that each column is a solution to the

    system and the columns are linearly independent. Since det(M) = ed1+d2+...+dnx = 0 for all

    x, the columns are linearly independent. Consider the ith column of M: Yi =

    0...

    edix

    ...

    0

    . Then,

    Yi =

    0...

    diedix

    ..

    .0

    and DYi =

    0...

    diedix

    ..

    .0

    , so Yi = DYi and Yi is a solution. Since this is true for

    all i, M is a matrix of fundamental solutions.

    27. (AB) =

    4e2x + 8e2x 2ex 2xex 8x 4e4x

    2ex + 4x 2ex 2xex + e3x + 3xe3x

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    6.2 Homogeneous Systems with Constant Coefficients - Diagonalizable

    3. From before, the eigenvalues are 2

    3 and 23, with basis eigenvectors

    32

    1

    and

    32

    1

    ,

    respectively. Therefore, the general solution to Y = AY is

    c1

    32 e

    23x

    e23x

    + c2

    32 e

    3

    2

    e3

    2

    =

    c132 e23x c232 e

    3

    2

    c1e23x + c2e

    3

    2

    5. The eigenvalues are 1, 2, and 3, with corresponding basis eigenvectors

    0

    1

    0

    ,

    1

    22

    ,

    1

    11

    ,

    respectively. Therefore, the general solution to Y = AY is

    c1

    0

    ex

    0

    + c2 e2x

    2e2x2e2x

    + c3 e3x

    e3xe3x

    = c2e

    2x + c3e3x

    c1ex 2c2e2x c3e3x2c2e2x c3e3x

    11. The eigenvalues are 1, i, and i with basis eigenvectors

    1

    0

    0

    ,

    0

    1

    i

    , and

    0

    1

    i

    , respectively.

    Therefore the general solution to Y = AY is

    c1

    ex

    0

    0

    + c2 0

    cos(x)

    sin(x) + c3

    0

    sin(x)

    cos(x)

    = c1e

    x

    c2 cos(x) + c3 sin(x)

    c2 sin(x) + c3 cos(x)

    15. Y(0) =

    0

    1

    1

    =

    c2 + c3

    c1 2c2 c32c2 c3

    = c1 = 2, c2 = 1, and c3 = 1. So, the solution is

    Y(x) =

    e2x e3x2ex

    2e2x + e3x

    2e2x + e3x

    22. The eigenvalues are solutions to 0 = 216 9 = 2 25 = ( 5)( +5), so the eigenvalues

    are 5. The corresponding basis eigenvectors are

    3

    1

    and

    1

    3

    . Therefore the general

    solution is

    c1

    3e5x

    e5x

    + c2

    e5x

    3e5x

    =

    3c1e

    5x + c2e5x

    c1e5x 3c2e5x

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    25. The eigenvalues are 13i with corresponding basis eigenvectors

    3i

    1

    and

    3i

    1

    . The general

    solution is then

    c1 3ex sin(3x)

    ex

    cos(x)+ c2

    3ex cos(3x)

    ex

    sin(3x) =

    3c1ex sin(3x) + 3c2ex cos(3x)

    c1ex

    cos(3x) + c2ex

    sin(3x)

    28. Y =

    2 1 0

    3 4 0

    5 6 3

    Y. The eigenvalues are 1, 3 and 5 with basis eigenvectors

    22

    11

    ,

    0

    0

    1

    , and

    2

    6

    13

    . Thus, the general solution is

    2c1ex

    + 2c3e5x

    2c1ex + 6c3e

    5x

    11c1ex + c2e

    3x 13c3e5x

    Thus,

    5

    3

    4

    = Y(0) =

    2c1 + 2c32c1 + 6c3

    11c1 + c2 13c3

    = c3 = 1, c1 = 32 , c2 = 672 . So, the solution is 3e

    x

    + 2e5x

    3ex + 6e5x332 ex + 672 e3x 13e5x

    30. The conditions on the eigenvalues are that the real parts of the eigenvalue are strictly negative

    (< 0).

    6.3 Homogeneous Systems with Constant Coefficients - Nondiagonalizable

    17. The matrix has eigenvalue

    6 with multiplicity 2 and a single basis eigenvector 11. Using

    Schurs Theorem and the Schur Decomposition, we can use Theorem 9.7 to find an orthogonal

    matrix P so that PTAP is upper triangular. Using

    1

    1

    as the start, the matrix P found

    using Theorem 9.7 is

    P =

    12 12

    12

    12

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    with PT = P. Thus,U = PTAP =

    6 20 6

    . The system Z = U Z gives

    z1(t) =

    6z1(t) + 2z2(t)

    z2(t) = 6z2(t)

    which has general solution z2(t) = c2e6t, z1(t) = c1e6t + 2c2te6t or c1

    e6t

    0

    + c2

    2te6t

    e6t

    .

    Thus, the general solution to the original problem is P Z or

    12

    (c1 + c2)e

    6t + 2c2te6t

    (c1 c2)e6t + 2c2te6t

    Using the initial value Y(0) =

    10

    , we get the system of equations

    1

    0

    =

    12

    c1 + c2

    c1 c2

    Thus, c1 = c2 =22 . Therefore, the solution is

    x(t)

    y(t)

    =

    e6t + te6t

    te6t

    6.4 Nonhomogeneous Linear Systems

    1. Y =

    3 0

    8 1

    Y +

    2

    x

    . The eigenvalues of the matrix are 3 and 1, with basis eigenvectors

    1

    2

    and

    0

    1

    . Thus, the general solution to the homogeneous linear system is

    YH = c1e

    3x

    2c1

    e3x

    +c2

    ex

    and a matrix of fundamental solutions is M =

    e3x 0

    2e3x ex

    . Thus,

    M1 =

    e3x 0

    2ex ex

    and YP = M

    M1G(x)dx =

    e3x 0

    2e3x ex

    e3x 0

    2ex ex

    2

    x

    dx.

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    So,

    YP =

    e3x 0

    2e3x ex

    2e3x

    4ex + xex

    dx

    = e3x 0

    2e3x ex

    2

    3e3x

    4ex + xex ex

    =

    23

    193 + x

    Thus, the general solution is

    Y = YP + YH =

    23 + c1e3x

    193 + x + 2c1e3x + c2ex

    5. The eigenvalues are 1, 2, and 3, with corresponding basis eigenvectors

    0

    1

    0

    ,

    1

    22

    ,

    1

    11

    ,

    respectively. Therefore, the general solution to Y = AY is

    c1

    0

    ex

    0

    + c2

    e2x

    2e2x2e2x

    + c3

    e3x

    e3xe3x

    =

    c2e2x + c3e

    3x

    c1ex 2c2e2x c3e3x2c2e2x c3e3x

    and a matrix of fundamental solutions is M =

    0 e2x e3x

    ex 2e2x e3x0 2e2x e3x

    . Thus,

    M1 =

    0 ex exe2x 0 e2x2e3x 0 e3x

    and

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    Using the initial condition (1, 1) gives the system

    1 + c1 + c2 = 1

    1 + 2c1 c2 = 1

    leading to c1 = 23 , c2 = 23 and the solutionx(t)

    y(t)

    =

    t + 1 + 23e

    4t 23ett 1 + 43e4t + 23et

    9 Inner Product Spaces

    9.1 Inner Product Spaces

    6. < v,u >= 0,

    ||v

    ||= ,

    ||u

    ||= , The angle between u and v is 2 .

    7. < f, g >=

    ba

    f(x)g(x)dx =

    ba

    g(x)f(x)dx =< g,f >

    < f+g,h >=

    ba

    (f(x)+g(x))h(x)dx =

    ba

    f(x)h(x)dx+

    ba

    g(x)h(x)dx =< f,h > + < g,h >

    < cf, g >=

    ba

    cf(x)g(x)dx = c

    ba

    f(x)g(x)dx = c < f, g >

    < f, f >=

    ba

    f2(x)dx 0 for all f andba

    f2(x)dx = 0 ifff(x) = 0 for all x.

    8. < v,u >= a1w1b1 + a2w2b2 + . . . + anwnbn =< u, v >

    < v + u, w >= (a1 + b1)w1c1 + (a2 + b2)w2c2 + . . . + (an + bn)wncn = a1w1c1 + . . . + anwncn +b1w1c1 + . . . + bnwncn =< v, w > + < u, w >

    < cv, u >= ca1w1b1 + ca2w2b2 + . . . + canwnbn = c < v, u >

    < v, v >= w1a21 + w2a

    22 + . . . + wna

    2n 0, since wi > 0 for all i. < v, v >= 0 if and only if

    a2i = 0 for all i = ai = 0 for all i = v = 0.

    16. Let v be a nonzero vector in a inner product space (V, < , >)). Then ||v|| = < v, v > > 0and

    =

    < v, v >

    ||v

    ||2

    = 1

    so, v||v|| is a unit vector.

    18. 0

    sin(x) sin(2x)dx =

    0

    2sin2(x) cos(x)dx =2

    3sin3(x)

    0

    = 0

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    9. < 1, 1 >=

    11

    (1)(1)dx = 2, so v1 =12

    .

    w2 = x 1

    1

    x2

    dx

    12

    = x, v2 =w2||w2|| =

    32x.

    w3 = x2

    1

    1

    x2

    2dx 12

    1

    1

    x3

    3

    2dxx3

    2

    = x2

    1

    3

    , v3 =w3

    ||w3||= 3

    5

    22(x2

    1

    3

    )

    13. Showing the matrix is orthogonal is equivalent to showing that {v1 =

    cos

    sin

    , v2 =

    sin

    cos

    }

    is an orthonormal basis for R2.

    v1 v1 = cos2 + sin2 = 1,v1 v2 = cos sin + sin cos = 0, andv2 v2 = sin2 + cos2 = 1.Thus, the set is an orthonormal basis and the matrix is orthogonal.