Problem 1. Let V = R 3 V = \mathbb{R}^3 V = R 3 and W = { ( x , y , z ) ∈ R 3 : x − y + z = 0 } W = \{(x, y, z) \in \mathbb{R}^3 : x - y + z = 0\} W = {( x , y , z ) ∈ R 3 : x − y + z = 0 } . Show that W W W is a subspace of V V V and find its dimension.
Solution W W W is non-empty since 0 = ( 0 , 0 , 0 ) ∈ W \mathbf{0} = (0, 0, 0) \in W 0 = ( 0 , 0 , 0 ) ∈ W . If ( x 1 , y 1 , z 1 ) , ( x 2 , y 2 , z 2 ) ∈ W (x_1, y_1, z_1), (x_2, y_2, z_2) \in W ( x 1 , y 1 , z 1 ) , ( x 2 , y 2 , z 2 ) ∈ W Then ( x 1 − y 1 + z 1 ) + ( x 2 − y 2 + z 2 ) = 0 + 0 = 0 (x_1 - y_1 + z_1) + (x_2 - y_2 + z_2) = 0 + 0 = 0 ( x 1 − y 1 + z 1 ) + ( x 2 − y 2 + z 2 ) = 0 + 0 = 0 So their sum is in W W W . Similarly, α ( x − y + z ) = 0 \alpha(x - y + z) = 0 α ( x − y + z ) = 0 for any scalar α \alpha α . Hence W W W is a subspace.
W W W is defined by one linear equation, so dim ( W ) = 3 − 1 = 2 \dim(W) = 3 - 1 = 2 dim ( W ) = 3 − 1 = 2 . A basis is { ( 1 , 1 , 0 ) , ( − 1 , 0 , 1 ) } \{(1, 1, 0), (-1, 0, 1)\} {( 1 , 1 , 0 ) , ( − 1 , 0 , 1 )} .
If you get this wrong, revise: Section 1.3 (Subspace Criterion).
Problem 2. Is the set S = { ( x , y ) ∈ R 2 : x y = 0 } S = \{(x, y) \in \mathbb{R}^2 : xy = 0\} S = {( x , y ) ∈ R 2 : x y = 0 } a subspace of R 2 \mathbb{R}^2 R 2 ?
Solution No. ( 1 , 0 ) ∈ S (1, 0) \in S ( 1 , 0 ) ∈ S and ( 0 , 1 ) ∈ S (0, 1) \in S ( 0 , 1 ) ∈ S But ( 1 , 0 ) + ( 0 , 1 ) = ( 1 , 1 ) ∉ S (1, 0) + (0, 1) = (1, 1) \notin S ( 1 , 0 ) + ( 0 , 1 ) = ( 1 , 1 ) ∈ / S since 1 ⋅ 1 ≠ 0 1 \cdot 1 \neq 0 1 ⋅ 1 = 0 . S S S is not closed under addition.
If you get this wrong, revise: Section 1.3 (Subspace Criterion).
Problem 3. Determine whether the set { 1 − x , 1 + x , x 2 } \{1 - x, 1 + x, x^2\} { 1 − x , 1 + x , x 2 } is linearly independent in P 2 ( R ) \mathcal{P}_2(\mathbb{R}) P 2 ( R ) .
Solution Suppose a ( 1 − x ) + b ( 1 + x ) + c x 2 = 0 a(1 - x) + b(1 + x) + cx^2 = 0 a ( 1 − x ) + b ( 1 + x ) + c x 2 = 0 as a polynomial. Then ( a + b ) + ( − a + b ) x + c x 2 = 0 (a + b) + (-a + b)x + cx^2 = 0 ( a + b ) + ( − a + b ) x + c x 2 = 0 So a + b = 0 a + b = 0 a + b = 0 , − a + b = 0 -a + b = 0 − a + b = 0 , c = 0 c = 0 c = 0 . From the first two equations: 2 a = 0 2a = 0 2 a = 0 So a = 0 a = 0 a = 0 Then b = 0 b = 0 b = 0 . Since a = b = c = 0 a = b = c = 0 a = b = c = 0 The set is linearly independent.
If you get this wrong, revise: Section 2.1 (Linear Independence).
Problem 4. Find a basis for the column space of
A = ( 1 2 1 4 2 4 0 6 3 6 1 10 ) A = \begin{pmatrix} 1 & 2 & 1 & 4 \\ 2 & 4 & 0 & 6 \\ 3 & 6 & 1 & 10 \end{pmatrix} A = 1 2 3 2 4 6 1 0 1 4 6 10
Solution Row-reduce A A A :
( 1 2 1 4 2 4 0 6 3 6 1 10 ) → R 2 − 2 R 1 , R 3 − 3 R 1 ( 1 2 1 4 0 0 − 2 − 2 0 0 − 2 − 2 ) → R 3 − R 2 ( 1 2 1 4 0 0 − 2 − 2 0 0 0 0 ) \begin{pmatrix} 1 & 2 & 1 & 4 \\ 2 & 4 & 0 & 6 \\ 3 & 6 & 1 & 10 \end{pmatrix} \xrightarrow{R_2 - 2R_1, R_3 - 3R_1} \begin{pmatrix} 1 & 2 & 1 & 4 \\ 0 & 0 & -2 & -2 \\ 0 & 0 & -2 & -2 \end{pmatrix} \xrightarrow{R_3 - R_2} \begin{pmatrix} 1 & 2 & 1 & 4 \\ 0 & 0 & -2 & -2 \\ 0 & 0 & 0 & 0 \end{pmatrix} 1 2 3 2 4 6 1 0 1 4 6 10 R 2 − 2 R 1 , R 3 − 3 R 1 1 0 0 2 0 0 1 − 2 − 2 4 − 2 − 2 R 3 − R 2 1 0 0 2 0 0 1 − 2 0 4 − 2 0
Pivots are in columns 1 and 3. A basis for c o l ( A ) \mathrm{col}(A) col ( A ) is { ( 1 , 2 , 3 ) , ( 1 , 0 , 1 ) } \{(1, 2, 3), (1, 0, 1)\} {( 1 , 2 , 3 ) , ( 1 , 0 , 1 )} (the pivot columns of the original A A A ). dim ( c o l ( A ) ) = 2 \dim(\mathrm{col}(A)) = 2 dim ( col ( A )) = 2 .
If you get this wrong, revise: Section 2.7 (Worked Examples).
Problem 5. Let U = s p a n { ( 1 , 0 , 1 ) , ( 0 , 1 , 1 ) } U = \mathrm{span}\{(1, 0, 1), (0, 1, 1)\} U = span {( 1 , 0 , 1 ) , ( 0 , 1 , 1 )} and W = s p a n { ( 1 , 1 , 0 ) } W = \mathrm{span}\{(1, 1, 0)\} W = span {( 1 , 1 , 0 )} in R 3 \mathbb{R}^3 R 3 . Verify the dimension formula dim ( U + W ) = dim ( U ) + dim ( W ) − dim ( U ∩ W ) \dim(U + W) = \dim(U) + \dim(W) - \dim(U \cap W) dim ( U + W ) = dim ( U ) + dim ( W ) − dim ( U ∩ W ) .
Solution dim ( U ) = 2 \dim(U) = 2 dim ( U ) = 2 (the two spanning vectors are linearly independent), dim ( W ) = 1 \dim(W) = 1 dim ( W ) = 1 . Since dim ( U ) + dim ( W ) = 3 = dim ( R 3 ) \dim(U) + \dim(W) = 3 = \dim(\mathbb{R}^3) dim ( U ) + dim ( W ) = 3 = dim ( R 3 ) We have U + W = R 3 U + W = \mathbb{R}^3 U + W = R 3 So dim ( U + W ) = 3 \dim(U + W) = 3 dim ( U + W ) = 3 . By the dimension formula: dim ( U ∩ W ) = 2 + 1 − 3 = 0 \dim(U \cap W) = 2 + 1 - 3 = 0 dim ( U ∩ W ) = 2 + 1 − 3 = 0 So U ∩ W = { 0 } U \cap W = \{\mathbf{0}\} U ∩ W = { 0 } .
We can verify directly: if a ( 1 , 0 , 1 ) + b ( 0 , 1 , 1 ) = c ( 1 , 1 , 0 ) a(1,0,1) + b(0,1,1) = c(1,1,0) a ( 1 , 0 , 1 ) + b ( 0 , 1 , 1 ) = c ( 1 , 1 , 0 ) Then a = c a = c a = c , b = c b = c b = c , a + b = 0 a + b = 0 a + b = 0 Giving c = 0 c = 0 c = 0 So only the zero vector is in the intersection.
If you get this wrong, revise: Section 2.5 (Dimension Formula).
Problem 6. Compute det ( A ) \det(A) det ( A ) using cofactor expansion where
A = ( 2 0 1 3 0 1 2 0 1 0 0 2 0 3 0 1 ) A = \begin{pmatrix} 2 & 0 & 1 & 3 \\ 0 & 1 & 2 & 0 \\ 1 & 0 & 0 & 2 \\ 0 & 3 & 0 & 1 \end{pmatrix} A = 2 0 1 0 0 1 0 3 1 2 0 0 3 0 2 1
Solution Expand along the second column (which has the most zeros):
det ( A ) = − 1 ⋅ det ( 2 1 3 1 0 2 0 0 1 ) + ( − 1 ) 4 + 2 ⋅ 3 ⋅ det ( 2 0 1 0 1 2 1 0 0 ) \det(A) = -1 \cdot \det\begin{pmatrix} 2 & 1 & 3 \\ 1 & 0 & 2 \\ 0 & 0 & 1 \end{pmatrix} + (-1)^{4+2} \cdot 3 \cdot \det\begin{pmatrix} 2 & 0 & 1 \\ 0 & 1 & 2 \\ 1 & 0 & 0 \end{pmatrix} det ( A ) = − 1 ⋅ det 2 1 0 1 0 0 3 2 1 + ( − 1 ) 4 + 2 ⋅ 3 ⋅ det 2 0 1 0 1 0 1 2 0
For the first 3 × 3 3 \times 3 3 × 3 : expand along row 3: 1 ⋅ ( 2 ⋅ 0 − 1 ⋅ 1 ) = − 1 1 \cdot (2 \cdot 0 - 1 \cdot 1) = -1 1 ⋅ ( 2 ⋅ 0 − 1 ⋅ 1 ) = − 1 .
For the second 3 × 3 3 \times 3 3 × 3 : expand along row 3: 1 ⋅ ( 0 ⋅ 2 − 1 ⋅ 1 ) = − 1 1 \cdot (0 \cdot 2 - 1 \cdot 1) = -1 1 ⋅ ( 0 ⋅ 2 − 1 ⋅ 1 ) = − 1 .
det ( A ) = − ( − 1 ) + 3 ( − 1 ) = 1 − 3 = − 2 \det(A) = -(-1) + 3(-1) = 1 - 3 = -2 det ( A ) = − ( − 1 ) + 3 ( − 1 ) = 1 − 3 = − 2 .
If you get this wrong, revise: Section 3.4 (Determinants).
Problem 7. Show that if A A A is skew-symmetric (A T = − A A^T = -A A T = − A ) and n n n is odd, then det ( A ) = 0 \det(A) = 0 det ( A ) = 0 .
Solution det ( A ) = det ( A T ) = det ( − A ) = ( − 1 ) n det ( A ) = − det ( A ) \det(A) = \det(A^T) = \det(-A) = (-1)^n \det(A) = -\det(A) det ( A ) = det ( A T ) = det ( − A ) = ( − 1 ) n det ( A ) = − det ( A ) (since n n n is odd). Therefore det ( A ) = − det ( A ) \det(A) = -\det(A) det ( A ) = − det ( A ) So 2 det ( A ) = 0 2\det(A) = 0 2 det ( A ) = 0 Giving det ( A ) = 0 \det(A) = 0 det ( A ) = 0 .
If you get this wrong, revise: Section 3.5 (Properties of Determinants).
Problem 8. Use the adjugate formula to find the inverse of
A = ( 2 0 1 1 1 0 0 1 3 ) A = \begin{pmatrix} 2 & 0 & 1 \\ 1 & 1 & 0 \\ 0 & 1 & 3 \end{pmatrix} A = 2 1 0 0 1 1 1 0 3
Solution det ( A ) = 2 ( 3 − 0 ) − 0 + 1 ( 1 − 0 ) = 6 + 1 = 7 \det(A) = 2(3 - 0) - 0 + 1(1 - 0) = 6 + 1 = 7 det ( A ) = 2 ( 3 − 0 ) − 0 + 1 ( 1 − 0 ) = 6 + 1 = 7 .
Cofactors: C 11 = + 3 C_{11} = +3 C 11 = + 3 , C 12 = − 3 C_{12} = -3 C 12 = − 3 , C 13 = + 1 C_{13} = +1 C 13 = + 1 C 21 = + 1 C_{21} = +1 C 21 = + 1 , C 22 = + 6 C_{22} = +6 C 22 = + 6 , C 23 = − 2 C_{23} = -2 C 23 = − 2 C 31 = − 1 C_{31} = -1 C 31 = − 1 , C 32 = + 1 C_{32} = +1 C 32 = + 1 , C 33 = + 2 C_{33} = +2 C 33 = + 2
a d j ( A ) = ( 3 1 − 1 − 3 6 1 1 − 2 2 ) \mathrm{adj}(A) = \begin{pmatrix} 3 & 1 & -1 \\ -3 & 6 & 1 \\ 1 & -2 & 2 \end{pmatrix} adj ( A ) = 3 − 3 1 1 6 − 2 − 1 1 2
A − 1 = 1 7 ( 3 1 − 1 − 3 6 1 1 − 2 2 ) A^{-1} = \frac{1}{7}\begin{pmatrix} 3 & 1 & -1 \\ -3 & 6 & 1 \\ 1 & -2 & 2 \end{pmatrix} A − 1 = 7 1 3 − 3 1 1 6 − 2 − 1 1 2
If you get this wrong, revise: Section 3.6 (Adjugate and Inverse Formula).
Problem 9. Solve the system by Gaussian elimination:
x + 2 y − z = 3 2 x + 5 y + z = 8 − x + y + 4 z = 2 \begin{aligned} x + 2y - z &= 3 \\ 2x + 5y + z &= 8 \\ -x + y + 4z &= 2 \end{aligned} x + 2 y − z 2 x + 5 y + z − x + y + 4 z = 3 = 8 = 2
Solution ( 1 2 − 1 3 2 5 1 8 − 1 1 4 2 ) → R 2 − 2 R 1 , R 3 + R 1 ( 1 2 − 1 3 0 1 3 2 0 3 3 5 ) \begin{pmatrix} 1 & 2 & -1 & 3 \\ 2 & 5 & 1 & 8 \\ -1 & 1 & 4 & 2 \end{pmatrix} \xrightarrow{R_2 - 2R_1, R_3 + R_1} \begin{pmatrix} 1 & 2 & -1 & 3 \\ 0 & 1 & 3 & 2 \\ 0 & 3 & 3 & 5 \end{pmatrix} 1 2 − 1 2 5 1 − 1 1 4 3 8 2 R 2 − 2 R 1 , R 3 + R 1 1 0 0 2 1 3 − 1 3 3 3 2 5
→ R 3 − 3 R 2 ( 1 2 − 1 3 0 1 3 2 0 0 − 6 − 1 ) \xrightarrow{R_3 - 3R_2} \begin{pmatrix} 1 & 2 & -1 & 3 \\ 0 & 1 & 3 & 2 \\ 0 & 0 & -6 & -1 \end{pmatrix} R 3 − 3 R 2 1 0 0 2 1 0 − 1 3 − 6 3 2 − 1
From row 3: − 6 z = − 1 -6z = -1 − 6 z = − 1 So z = 1 / 6 z = 1/6 z = 1/6 . From row 2: y + 3 ( 1 / 6 ) = 2 y + 3(1/6) = 2 y + 3 ( 1/6 ) = 2 So y = 3 / 2 y = 3/2 y = 3/2 . From row 1: x + 2 ( 3 / 2 ) − 1 / 6 = 3 x + 2(3/2) - 1/6 = 3 x + 2 ( 3/2 ) − 1/6 = 3 So x = 3 − 3 + 1 / 6 = 1 / 6 x = 3 - 3 + 1/6 = 1/6 x = 3 − 3 + 1/6 = 1/6 .
Solution: x = 1 / 6 x = 1/6 x = 1/6 , y = 3 / 2 y = 3/2 y = 3/2 , z = 1 / 6 z = 1/6 z = 1/6 .
If you get this wrong, revise: Section 4.1 (Gaussian Elimination).
Problem 10. Determine whether the following system is consistent using the Rouché—Capelli theorem:
x + y + z = 1 2 x + 2 y + 2 z = 3 x − y + z = 0 \begin{aligned} x + y + z &= 1 \\ 2x + 2y + 2z &= 3 \\ x - y + z &= 0 \end{aligned} x + y + z 2 x + 2 y + 2 z x − y + z = 1 = 3 = 0
Solution [ A ∣ b ] = ( 1 1 1 1 2 2 2 3 1 − 1 1 0 ) → R 2 − 2 R 1 , R 3 − R 1 ( 1 1 1 1 0 0 0 1 0 − 2 0 − 1 ) [A \mid \mathbf{b}] = \begin{pmatrix} 1 & 1 & 1 & 1 \\ 2 & 2 & 2 & 3 \\ 1 & -1 & 1 & 0 \end{pmatrix} \xrightarrow{R_2 - 2R_1, R_3 - R_1} \begin{pmatrix} 1 & 1 & 1 & 1 \\ 0 & 0 & 0 & 1 \\ 0 & -2 & 0 & -1 \end{pmatrix} [ A ∣ b ] = 1 2 1 1 2 − 1 1 2 1 1 3 0 R 2 − 2 R 1 , R 3 − R 1 1 0 0 1 0 − 2 1 0 0 1 1 − 1
r a n k ( A ) = 2 \mathrm{rank}(A) = 2 rank ( A ) = 2 but r a n k ( [ A ∣ b ] ) = 3 \mathrm{rank}([A \mid \mathbf{b}]) = 3 rank ([ A ∣ b ]) = 3 (the row [ 0 0 0 1 ] [0\ 0\ 0\ 1] [ 0 0 0 1 ] is Non-zero). Since r a n k ( A ) ≠ r a n k ( [ A ∣ b ] ) \mathrm{rank}(A) \neq \mathrm{rank}([A \mid \mathbf{b}]) rank ( A ) = rank ([ A ∣ b ]) The system is inconsistent.
If you get this wrong, revise: Section 4.2 (Rouché—Capelli Theorem).
Problem 11. Find the LU decomposition of
A = ( 1 2 − 1 2 5 0 − 1 0 3 ) A = \begin{pmatrix} 1 & 2 & -1 \\ 2 & 5 & 0 \\ -1 & 0 & 3 \end{pmatrix} A = 1 2 − 1 2 5 0 − 1 0 3
Solution m 21 = 2 / 1 = 2 m_{21} = 2/1 = 2 m 21 = 2/1 = 2 , m 31 = − 1 / 1 = − 1 m_{31} = -1/1 = -1 m 31 = − 1/1 = − 1 :
( 1 2 − 1 0 1 2 0 2 2 ) \begin{pmatrix} 1 & 2 & -1 \\ 0 & 1 & 2 \\ 0 & 2 & 2 \end{pmatrix} 1 0 0 2 1 2 − 1 2 2
m 32 = 2 / 1 = 2 m_{32} = 2/1 = 2 m 32 = 2/1 = 2 :
U = ( 1 2 − 1 0 1 2 0 0 − 2 ) , L = ( 1 0 0 2 1 0 − 1 2 1 ) U = \begin{pmatrix} 1 & 2 & -1 \\ 0 & 1 & 2 \\ 0 & 0 & -2 \end{pmatrix}, \quad L = \begin{pmatrix} 1 & 0 & 0 \\ 2 & 1 & 0 \\ -1 & 2 & 1 \end{pmatrix} U = 1 0 0 2 1 0 − 1 2 − 2 , L = 1 2 − 1 0 1 2 0 0 1
Verify: L U = ( 1 0 0 2 1 0 − 1 2 1 ) ( 1 2 − 1 0 1 2 0 0 − 2 ) = ( 1 2 − 1 2 5 0 − 1 0 3 ) = A LU = \begin{pmatrix} 1 & 0 & 0 \\ 2 & 1 & 0 \\ -1 & 2 & 1 \end{pmatrix}\begin{pmatrix} 1 & 2 & -1 \\ 0 & 1 & 2 \\ 0 & 0 & -2 \end{pmatrix} = \begin{pmatrix} 1 & 2 & -1 \\ 2 & 5 & 0 \\ -1 & 0 & 3 \end{pmatrix} = A LU = 1 2 − 1 0 1 2 0 0 1 1 0 0 2 1 0 − 1 2 − 2 = 1 2 − 1 2 5 0 − 1 0 3 = A . ■ \blacksquare ■
If you get this wrong, revise: Section 4.3 (LU Decomposition).
Problem 12. Find the least squares solution to the system A x = b A\mathbf{x} = \mathbf{b} A x = b where
A = ( 1 0 1 1 1 2 ) , b = ( 0 1 1 ) A = \begin{pmatrix} 1 & 0 \\ 1 & 1 \\ 1 & 2 \end{pmatrix}, \quad \mathbf{b} = \begin{pmatrix} 0 \\ 1 \\ 1 \end{pmatrix} A = 1 1 1 0 1 2 , b = 0 1 1
Solution A T A = ( 3 3 3 5 ) A^T A = \begin{pmatrix} 3 & 3 \\ 3 & 5 \end{pmatrix} A T A = ( 3 3 3 5 ) , A T b = ( 2 3 ) A^T \mathbf{b} = \begin{pmatrix} 2 \\ 3 \end{pmatrix} A T b = ( 2 3 ) .
det ( A T A ) = 15 − 9 = 6 \det(A^T A) = 15 - 9 = 6 det ( A T A ) = 15 − 9 = 6 , ( A T A ) − 1 = 1 6 ( 5 − 3 − 3 3 ) (A^T A)^{-1} = \frac{1}{6}\begin{pmatrix} 5 & -3 \\ -3 & 3 \end{pmatrix} ( A T A ) − 1 = 6 1 ( 5 − 3 − 3 3 )
x ^ = 1 6 ( 5 − 3 − 3 3 ) ( 2 3 ) = 1 6 ( 10 − 9 − 6 + 9 ) = 1 6 ( 1 3 ) = ( 1 / 6 1 / 2 ) \hat{\mathbf{x}} = \frac{1}{6}\begin{pmatrix} 5 & -3 \\ -3 & 3 \end{pmatrix}\begin{pmatrix} 2 \\ 3 \end{pmatrix} = \frac{1}{6}\begin{pmatrix} 10 - 9 \\ -6 + 9 \end{pmatrix} = \frac{1}{6}\begin{pmatrix} 1 \\ 3 \end{pmatrix} = \begin{pmatrix} 1/6 \\ 1/2 \end{pmatrix} x ^ = 6 1 ( 5 − 3 − 3 3 ) ( 2 3 ) = 6 1 ( 10 − 9 − 6 + 9 ) = 6 1 ( 1 3 ) = ( 1/6 1/2 )
The least squares solution is a = 1 / 6 a = 1/6 a = 1/6 , b = 1 / 2 b = 1/2 b = 1/2 .
If you get this wrong, revise: Section 4.5 (Least Squares Solutions).
Problem 13. Find the eigenvalues and a basis for each eigenspace of
A = ( 2 1 0 0 2 1 0 0 2 ) A = \begin{pmatrix} 2 & 1 & 0 \\ 0 & 2 & 1 \\ 0 & 0 & 2 \end{pmatrix} A = 2 0 0 1 2 0 0 1 2
Is A A A diagonalisable?
Solution det ( A − λ I ) = ( 2 − λ ) 3 \det(A - \lambda I) = (2 - \lambda)^3 det ( A − λ I ) = ( 2 − λ ) 3 So λ = 2 \lambda = 2 λ = 2 with algebraic multiplicity 3.
A − 2 I = ( 0 1 0 0 0 1 0 0 0 ) A - 2I = \begin{pmatrix} 0 & 1 & 0 \\ 0 & 0 & 1 \\ 0 & 0 & 0 \end{pmatrix} A − 2 I = 0 0 0 1 0 0 0 1 0 Which has rank 2. The null space is spanned by ( 1 , 0 , 0 ) T (1, 0, 0)^T ( 1 , 0 , 0 ) T . So the geometric multiplicity is 1.
Since the geometric multiplicity (1) does not equal the algebraic multiplicity (3), A A A is not Diagonalisable. Its Jordan form is J = A J = A J = A itself (a single 3 × 3 3 \times 3 3 × 3 Jordan block).
If you get this wrong, revise: Section 5.3 (Diagonalisation) and Section 5.5 (Jordan Normal Form).
Problem 14. Diagonalise the matrix
A = ( 2 0 0 0 3 − 1 0 − 1 3 ) A = \begin{pmatrix} 2 & 0 & 0 \\ 0 & 3 & -1 \\ 0 & -1 & 3 \end{pmatrix} A = 2 0 0 0 3 − 1 0 − 1 3
Solution det ( A − λ I ) = ( 2 − λ ) [ ( 3 − λ ) 2 − 1 ] = ( 2 − λ ) ( λ 2 − 6 λ + 8 ) = ( 2 − λ ) ( λ − 2 ) ( λ − 4 ) \det(A - \lambda I) = (2 - \lambda)[(3-\lambda)^2 - 1] = (2-\lambda)(\lambda^2 - 6\lambda + 8) = (2-\lambda)(\lambda-2)(\lambda-4) det ( A − λ I ) = ( 2 − λ ) [( 3 − λ ) 2 − 1 ] = ( 2 − λ ) ( λ 2 − 6 λ + 8 ) = ( 2 − λ ) ( λ − 2 ) ( λ − 4 ) .
Eigenvalues: λ 1 = 2 \lambda_1 = 2 λ 1 = 2 (algebraic multiplicity 2), λ 2 = 4 \lambda_2 = 4 λ 2 = 4 (algebraic multiplicity 1).
For λ 1 = 2 \lambda_1 = 2 λ 1 = 2 : A − 2 I = ( 0 0 0 0 1 − 1 0 − 1 1 ) → ( 0 1 − 1 0 0 0 0 0 0 ) A - 2I = \begin{pmatrix} 0 & 0 & 0 \\ 0 & 1 & -1 \\ 0 & -1 & 1 \end{pmatrix} \to \begin{pmatrix} 0 & 1 & -1 \\ 0 & 0 & 0 \\ 0 & 0 & 0 \end{pmatrix} A − 2 I = 0 0 0 0 1 − 1 0 − 1 1 → 0 0 0 1 0 0 − 1 0 0 . Eigenspace basis: { ( 1 , 0 , 0 ) , ( 0 , 1 , 1 ) } \{(1, 0, 0), (0, 1, 1)\} {( 1 , 0 , 0 ) , ( 0 , 1 , 1 )} . Geometric multiplicity = 2.
For λ 2 = 4 \lambda_2 = 4 λ 2 = 4 : A − 4 I = ( − 2 0 0 0 − 1 − 1 0 − 1 − 1 ) → ( 1 0 0 0 1 1 0 0 0 ) A - 4I = \begin{pmatrix} -2 & 0 & 0 \\ 0 & -1 & -1 \\ 0 & -1 & -1 \end{pmatrix} \to \begin{pmatrix} 1 & 0 & 0 \\ 0 & 1 & 1 \\ 0 & 0 & 0 \end{pmatrix} A − 4 I = − 2 0 0 0 − 1 − 1 0 − 1 − 1 → 1 0 0 0 1 0 0 1 0 . Eigenspace basis: { ( 0 , − 1 , 1 ) } \{(0, -1, 1)\} {( 0 , − 1 , 1 )} . Geometric multiplicity = 1.
Since 2 + 1 = 3 = n 2 + 1 = 3 = n 2 + 1 = 3 = n , A A A is diagonalisable:
P = ( 1 0 0 0 1 − 1 0 1 1 ) , D = ( 2 0 0 0 2 0 0 0 4 ) P = \begin{pmatrix} 1 & 0 & 0 \\ 0 & 1 & -1 \\ 0 & 1 & 1 \end{pmatrix}, \quad D = \begin{pmatrix} 2 & 0 & 0 \\ 0 & 2 & 0 \\ 0 & 0 & 4 \end{pmatrix} P = 1 0 0 0 1 1 0 − 1 1 , D = 2 0 0 0 2 0 0 0 4
If you get this wrong, revise: Section 5.3 (Diagonalisation).
Problem 15. Use the Cayley—Hamilton theorem to express A 3 A^3 A 3 as a linear combination of A 2 A^2 A 2 , A A A And I I I Where A = ( 1 2 − 1 3 ) A = \begin{pmatrix} 1 & 2 \\ -1 & 3 \end{pmatrix} A = ( 1 − 1 2 3 ) .
Solution det ( A − λ I ) = ( 1 − λ ) ( 3 − λ ) + 2 = λ 2 − 4 λ + 5 \det(A - \lambda I) = (1 - \lambda)(3 - \lambda) + 2 = \lambda^2 - 4\lambda + 5 det ( A − λ I ) = ( 1 − λ ) ( 3 − λ ) + 2 = λ 2 − 4 λ + 5 .
By Cayley—Hamilton: A 2 − 4 A + 5 I = 0 A^2 - 4A + 5I = 0 A 2 − 4 A + 5 I = 0 So A 2 = 4 A − 5 I A^2 = 4A - 5I A 2 = 4 A − 5 I .
A 3 = A ⋅ A 2 = A ( 4 A − 5 I ) = 4 A 2 − 5 A = 4 ( 4 A − 5 I ) − 5 A = 16 A − 20 I − 5 A = 11 A − 20 I A^3 = A \cdot A^2 = A(4A - 5I) = 4A^2 - 5A = 4(4A - 5I) - 5A = 16A - 20I - 5A = 11A - 20I A 3 = A ⋅ A 2 = A ( 4 A − 5 I ) = 4 A 2 − 5 A = 4 ( 4 A − 5 I ) − 5 A = 16 A − 20 I − 5 A = 11 A − 20 I .
A 3 = 11 ( 1 2 − 1 3 ) − 20 ( 1 0 0 1 ) = ( − 9 22 − 11 13 ) A^3 = 11\begin{pmatrix} 1 & 2 \\ -1 & 3 \end{pmatrix} - 20\begin{pmatrix} 1 & 0 \\ 0 & 1 \end{pmatrix} = \begin{pmatrix} -9 & 22 \\ -11 & 13 \end{pmatrix} A 3 = 11 ( 1 − 1 2 3 ) − 20 ( 1 0 0 1 ) = ( − 9 − 11 22 13 ) .
If you get this wrong, revise: Section 5.4 (Cayley—Hamilton Theorem).
Problem 16. Let T : R 3 → R 2 T : \mathbb{R}^3 \to \mathbb{R}^2 T : R 3 → R 2 be defined by T ( x , y , z ) = ( x + y , y + z ) T(x, y, z) = (x + y, y + z) T ( x , y , z ) = ( x + y , y + z ) . Find the matrix of T T T with respect to the standard bases, and verify the rank-nullity theorem.
Solution T ( 1 , 0 , 0 ) = ( 1 , 0 ) T(1, 0, 0) = (1, 0) T ( 1 , 0 , 0 ) = ( 1 , 0 ) , T ( 0 , 1 , 0 ) = ( 1 , 1 ) T(0, 1, 0) = (1, 1) T ( 0 , 1 , 0 ) = ( 1 , 1 ) , T ( 0 , 0 , 1 ) = ( 0 , 1 ) T(0, 0, 1) = (0, 1) T ( 0 , 0 , 1 ) = ( 0 , 1 ) .
[ T ] E = ( 1 1 0 0 1 1 ) [T]_{\mathcal{E}} = \begin{pmatrix} 1 & 1 & 0 \\ 0 & 1 & 1 \end{pmatrix} [ T ] E = ( 1 0 1 1 0 1 ) .
ker ( T ) = { ( x , y , z ) : x + y = 0 , y + z = 0 } = { ( t , − t , t ) : t ∈ R } \ker(T) = \{(x, y, z) : x + y = 0, y + z = 0\} = \{(t, -t, t) : t \in \mathbb{R}\} ker ( T ) = {( x , y , z ) : x + y = 0 , y + z = 0 } = {( t , − t , t ) : t ∈ R } So dim ( ker ( T ) ) = 1 \dim(\ker(T)) = 1 dim ( ker ( T )) = 1 .
i m ( T ) = s p a n { ( 1 , 0 ) , ( 1 , 1 ) } = R 2 \mathrm{im}(T) = \mathrm{span}\{(1, 0), (1, 1)\} = \mathbb{R}^2 im ( T ) = span {( 1 , 0 ) , ( 1 , 1 )} = R 2 So dim ( i m ( T ) ) = 2 \dim(\mathrm{im}(T)) = 2 dim ( im ( T )) = 2 .
Verify: dim ( ker ( T ) ) + dim ( i m ( T ) ) = 1 + 2 = 3 = dim ( R 3 ) \dim(\ker(T)) + \dim(\mathrm{im}(T)) = 1 + 2 = 3 = \dim(\mathbb{R}^3) dim ( ker ( T )) + dim ( im ( T )) = 1 + 2 = 3 = dim ( R 3 ) . ■ \blacksquare ■
If you get this wrong, revise: Section 6.4 (Rank-Nullity for Linear Maps).
Problem 17. Let V = R 3 V = \mathbb{R}^3 V = R 3 with the standard inner product. Find the orthogonal projection Of v = ( 1 , 2 , 3 ) \mathbf{v} = (1, 2, 3) v = ( 1 , 2 , 3 ) onto the plane W W W defined by x + y + z = 0 x + y + z = 0 x + y + z = 0 .
Solution A basis for W W W : { ( 1 , − 1 , 0 ) , ( 1 , 0 , − 1 ) } \{(1, -1, 0), (1, 0, -1)\} {( 1 , − 1 , 0 ) , ( 1 , 0 , − 1 )} . Apply Gram—Schmidt:
e 1 = 1 2 ( 1 , − 1 , 0 ) e_1 = \frac{1}{\sqrt{2}}(1, -1, 0) e 1 = 2 1 ( 1 , − 1 , 0 ) .
u 2 = ( 1 , 0 , − 1 ) − ⟨ ( 1 , 0 , − 1 ) , e 1 ⟩ e 1 = ( 1 , 0 , − 1 ) − 1 2 ⋅ 1 2 ( 1 , − 1 , 0 ) = ( 1 2 , 1 2 , − 1 ) \mathbf{u}_2 = (1, 0, -1) - \langle (1, 0, -1), e_1 \rangle e_1 = (1, 0, -1) - \frac{1}{\sqrt{2}} \cdot \frac{1}{\sqrt{2}}(1, -1, 0) = (\frac{1}{2}, \frac{1}{2}, -1) u 2 = ( 1 , 0 , − 1 ) − ⟨( 1 , 0 , − 1 ) , e 1 ⟩ e 1 = ( 1 , 0 , − 1 ) − 2 1 ⋅ 2 1 ( 1 , − 1 , 0 ) = ( 2 1 , 2 1 , − 1 ) .
∥ u 2 ∥ = 1 / 4 + 1 / 4 + 1 = 3 / 2 \lVert \mathbf{u}_2 \rVert = \sqrt{1/4 + 1/4 + 1} = \sqrt{3/2} ∥ u 2 ∥ = 1/4 + 1/4 + 1 = 3/2 So e 2 = 1 6 ( 1 , 1 , − 2 ) e_2 = \frac{1}{\sqrt{6}}(1, 1, -2) e 2 = 6 1 ( 1 , 1 , − 2 ) .
p r o j W ( v ) = ⟨ ( 1 , 2 , 3 ) , e 1 ⟩ e 1 + ⟨ ( 1 , 2 , 3 ) , e 2 ⟩ e 2 \mathrm{proj_W}(\mathbf{v}) = \langle (1,2,3), e_1 \rangle e_1 + \langle (1,2,3), e_2 \rangle e_2 pro j W ( v ) = ⟨( 1 , 2 , 3 ) , e 1 ⟩ e 1 + ⟨( 1 , 2 , 3 ) , e 2 ⟩ e 2
⟨ ( 1 , 2 , 3 ) , e 1 ⟩ = 1 2 ( 1 − 2 ) = − 1 2 \langle (1,2,3), e_1 \rangle = \frac{1}{\sqrt{2}}(1 - 2) = \frac{-1}{\sqrt{2}} ⟨( 1 , 2 , 3 ) , e 1 ⟩ = 2 1 ( 1 − 2 ) = 2 − 1
⟨ ( 1 , 2 , 3 ) , e 2 ⟩ = 1 6 ( 1 + 2 − 6 ) = − 3 6 \langle (1,2,3), e_2 \rangle = \frac{1}{\sqrt{6}}(1 + 2 - 6) = \frac{-3}{\sqrt{6}} ⟨( 1 , 2 , 3 ) , e 2 ⟩ = 6 1 ( 1 + 2 − 6 ) = 6 − 3
p r o j W ( v ) = − 1 2 ⋅ 1 2 ( 1 , − 1 , 0 ) + − 3 6 ⋅ 1 6 ( 1 , 1 , − 2 ) \mathrm{proj_W}(\mathbf{v}) = \frac{-1}{\sqrt{2}} \cdot \frac{1}{\sqrt{2}}(1, -1, 0) + \frac{-3}{\sqrt{6}} \cdot \frac{1}{\sqrt{6}}(1, 1, -2) pro j W ( v ) = 2 − 1 ⋅ 2 1 ( 1 , − 1 , 0 ) + 6 − 3 ⋅ 6 1 ( 1 , 1 , − 2 )
= − 1 2 ( 1 , − 1 , 0 ) − 1 2 ( 1 , 1 , − 2 ) = ( − 1 , 0 , 1 ) = -\frac{1}{2}(1, -1, 0) - \frac{1}{2}(1, 1, -2) = (-1, 0, 1) = − 2 1 ( 1 , − 1 , 0 ) − 2 1 ( 1 , 1 , − 2 ) = ( − 1 , 0 , 1 ) .
The orthogonal projection is ( − 1 , 0 , 1 ) (-1, 0, 1) ( − 1 , 0 , 1 ) . ■ \blacksquare ■
If you get this wrong, revise: Section 7.5 (Orthogonal Projection).
Problem 18. Prove the Cauchy—Schwarz inequality for R n \mathbb{R}^n R n directly: for any nonzero x , y ∈ R n \mathbf{x}, \mathbf{y} \in \mathbb{R}^n x , y ∈ R n Show that ∣ x ⋅ y ∣ ≤ ∥ x ∥ ∥ y ∥ \lvert\mathbf{x} \cdot \mathbf{y}\rvert \leq \lVert \mathbf{x} \rVert \lVert \mathbf{y} \rVert ∣ x ⋅ y ∣ ≤ ∥ x ∥ ∥ y ∥ And determine when equality holds.
Solution Consider the function f ( t ) = ∥ x + t y ∥ 2 = ∥ x ∥ 2 + 2 t ( x ⋅ y ) + t 2 ∥ y ∥ 2 f(t) = \lVert \mathbf{x} + t\mathbf{y} \rVert^2 = \lVert \mathbf{x} \rVert^2 + 2t(\mathbf{x} \cdot \mathbf{y}) + t^2 \lVert \mathbf{y} \rVert^2 f ( t ) = ∥ x + t y ∥ 2 = ∥ x ∥ 2 + 2 t ( x ⋅ y ) + t 2 ∥ y ∥ 2 .
Since f ( t ) ≥ 0 f(t) \geq 0 f ( t ) ≥ 0 for all t ∈ R t \in \mathbb{R} t ∈ R This quadratic in t t t has at most one real root, So its discriminant satisfies Δ ≤ 0 \Delta \leq 0 Δ ≤ 0 :
4 ( x ⋅ y ) 2 − 4 ∥ x ∥ 2 ∥ y ∥ 2 ≤ 0 4(\mathbf{x} \cdot \mathbf{y})^2 - 4\lVert \mathbf{x} \rVert^2 \lVert \mathbf{y} \rVert^2 \leq 0 4 ( x ⋅ y ) 2 − 4 ∥ x ∥ 2 ∥ y ∥ 2 ≤ 0
Therefore ( x ⋅ y ) 2 ≤ ∥ x ∥ 2 ∥ y ∥ 2 (\mathbf{x} \cdot \mathbf{y})^2 \leq \lVert \mathbf{x} \rVert^2 \lVert \mathbf{y} \rVert^2 ( x ⋅ y ) 2 ≤ ∥ x ∥ 2 ∥ y ∥ 2 And taking square roots gives the result.
Equality holds iff Δ = 0 \Delta = 0 Δ = 0 Which means f ( t ) f(t) f ( t ) has a double root, i.e., there exists t 0 t_0 t 0 such that x + t 0 y = 0 \mathbf{x} + t_0 \mathbf{y} = \mathbf{0} x + t 0 y = 0 Meaning x \mathbf{x} x and y \mathbf{y} y are linearly dependent.
If you get this wrong, revise: Section 7.2 (Cauchy—Schwarz Inequality).
Problem 19. Let A = ( 1 0 0 0 2 1 0 1 2 ) A = \begin{pmatrix} 1 & 0 & 0 \\ 0 & 2 & 1 \\ 0 & 1 & 2 \end{pmatrix} A = 1 0 0 0 2 1 0 1 2 . Verify the Cayley—Hamilton Theorem by explicitly computing p ( A ) p(A) p ( A ) .
Solution p ( λ ) = det ( A − λ I ) = ( 1 − λ ) [ ( 2 − λ ) 2 − 1 ] = ( 1 − λ ) ( λ 2 − 4 λ + 3 ) = ( 1 − λ ) ( λ − 1 ) ( λ − 3 ) p(\lambda) = \det(A - \lambda I) = (1 - \lambda)[(2-\lambda)^2 - 1] = (1-\lambda)(\lambda^2 - 4\lambda + 3) = (1-\lambda)(\lambda-1)(\lambda-3) p ( λ ) = det ( A − λ I ) = ( 1 − λ ) [( 2 − λ ) 2 − 1 ] = ( 1 − λ ) ( λ 2 − 4 λ + 3 ) = ( 1 − λ ) ( λ − 1 ) ( λ − 3 ) .
So p ( λ ) = − ( λ − 1 ) 2 ( λ − 3 ) = − ( λ 3 − 5 λ 2 + 7 λ − 3 ) p(\lambda) = -(\lambda-1)^2(\lambda-3) = -(\lambda^3 - 5\lambda^2 + 7\lambda - 3) p ( λ ) = − ( λ − 1 ) 2 ( λ − 3 ) = − ( λ 3 − 5 λ 2 + 7 λ − 3 ) .
p ( A ) = − ( A 3 − 5 A 2 + 7 A − 3 I ) p(A) = -(A^3 - 5A^2 + 7A - 3I) p ( A ) = − ( A 3 − 5 A 2 + 7 A − 3 I ) .
A 2 = ( 1 0 0 0 2 1 0 1 2 ) 2 = ( 1 0 0 0 5 4 0 4 5 ) A^2 = \begin{pmatrix} 1 & 0 & 0 \\ 0 & 2 & 1 \\ 0 & 1 & 2 \end{pmatrix}^2 = \begin{pmatrix} 1 & 0 & 0 \\ 0 & 5 & 4 \\ 0 & 4 & 5 \end{pmatrix} A 2 = 1 0 0 0 2 1 0 1 2 2 = 1 0 0 0 5 4 0 4 5
A 3 = A ⋅ A 2 = ( 1 0 0 0 2 1 0 1 2 ) ( 1 0 0 0 5 4 0 4 5 ) = ( 1 0 0 0 14 13 0 13 14 ) A^3 = A \cdot A^2 = \begin{pmatrix} 1 & 0 & 0 \\ 0 & 2 & 1 \\ 0 & 1 & 2 \end{pmatrix}\begin{pmatrix} 1 & 0 & 0 \\ 0 & 5 & 4 \\ 0 & 4 & 5 \end{pmatrix} = \begin{pmatrix} 1 & 0 & 0 \\ 0 & 14 & 13 \\ 0 & 13 & 14 \end{pmatrix} A 3 = A ⋅ A 2 = 1 0 0 0 2 1 0 1 2 1 0 0 0 5 4 0 4 5 = 1 0 0 0 14 13 0 13 14
p ( A ) = − ( 1 0 0 0 14 13 0 13 14 ) + 5 ( 1 0 0 0 5 4 0 4 5 ) − 7 ( 1 0 0 0 2 1 0 1 2 ) + 3 ( 1 0 0 0 1 0 0 0 1 ) p(A) = -\begin{pmatrix} 1 & 0 & 0 \\ 0 & 14 & 13 \\ 0 & 13 & 14 \end{pmatrix} + 5\begin{pmatrix} 1 & 0 & 0 \\ 0 & 5 & 4 \\ 0 & 4 & 5 \end{pmatrix} - 7\begin{pmatrix} 1 & 0 & 0 \\ 0 & 2 & 1 \\ 0 & 1 & 2 \end{pmatrix} + 3\begin{pmatrix} 1 & 0 & 0 \\ 0 & 1 & 0 \\ 0 & 0 & 1 \end{pmatrix} p ( A ) = − 1 0 0 0 14 13 0 13 14 + 5 1 0 0 0 5 4 0 4 5 − 7 1 0 0 0 2 1 0 1 2 + 3 1 0 0 0 1 0 0 0 1
= ( − 1 + 5 − 7 + 3 0 0 0 − 14 + 25 − 14 + 3 − 13 + 20 − 7 + 0 0 − 13 + 20 − 7 + 0 − 14 + 25 − 14 + 3 ) = ( 0 0 0 0 0 0 0 0 0 ) = \begin{pmatrix} -1+5-7+3 & 0 & 0 \\ 0 & -14+25-14+3 & -13+20-7+0 \\ 0 & -13+20-7+0 & -14+25-14+3 \end{pmatrix} = \begin{pmatrix} 0 & 0 & 0 \\ 0 & 0 & 0 \\ 0 & 0 & 0 \end{pmatrix} = − 1 + 5 − 7 + 3 0 0 0 − 14 + 25 − 14 + 3 − 13 + 20 − 7 + 0 0 − 13 + 20 − 7 + 0 − 14 + 25 − 14 + 3 = 0 0 0 0 0 0 0 0 0
So p ( A ) = 0 p(A) = 0 p ( A ) = 0 Confirming Cayley—Hamilton. ■ \blacksquare ■
If you get this wrong, revise: Section 5.4 (Cayley—Hamilton Theorem).
Problem 20. Let T : P 2 ( R ) → P 2 ( R ) T : \mathcal{P}_2(\mathbb{R}) \to \mathcal{P}_2(\mathbb{R}) T : P 2 ( R ) → P 2 ( R ) be defined by T ( p ) = p " T(p) = p" T ( p ) = p " (the derivative). Find the matrix of T T T with respect to the basis B = { 1 , x , x 2 } \mathcal{B} = \{1, x, x^2\} B = { 1 , x , x 2 } And determine ker ( T ) \ker(T) ker ( T ) and i m ( T ) \mathrm{im}(T) im ( T ) .
Solution T ( 1 ) = 0 = 0 ⋅ 1 + 0 ⋅ x + 0 ⋅ x 2 T(1) = 0 = 0 \cdot 1 + 0 \cdot x + 0 \cdot x^2 T ( 1 ) = 0 = 0 ⋅ 1 + 0 ⋅ x + 0 ⋅ x 2 So coordinates are ( 0 0 0 ) \begin{pmatrix} 0 \\ 0 \\ 0 \end{pmatrix} 0 0 0 .
T ( x ) = 1 = 1 ⋅ 1 + 0 ⋅ x + 0 ⋅ x 2 T(x) = 1 = 1 \cdot 1 + 0 \cdot x + 0 \cdot x^2 T ( x ) = 1 = 1 ⋅ 1 + 0 ⋅ x + 0 ⋅ x 2 So coordinates are ( 1 0 0 ) \begin{pmatrix} 1 \\ 0 \\ 0 \end{pmatrix} 1 0 0 .
T ( x 2 ) = 2 x = 0 ⋅ 1 + 2 ⋅ x + 0 ⋅ x 2 T(x^2) = 2x = 0 \cdot 1 + 2 \cdot x + 0 \cdot x^2 T ( x 2 ) = 2 x = 0 ⋅ 1 + 2 ⋅ x + 0 ⋅ x 2 So coordinates are ( 0 2 0 ) \begin{pmatrix} 0 \\ 2 \\ 0 \end{pmatrix} 0 2 0 .
[ T ] B = ( 0 1 0 0 0 2 0 0 0 ) [T]_{\mathcal{B}} = \begin{pmatrix} 0 & 1 & 0 \\ 0 & 0 & 2 \\ 0 & 0 & 0 \end{pmatrix} [ T ] B = 0 0 0 1 0 0 0 2 0
ker ( T ) = { p : p ′ = 0 } = s p a n { 1 } \ker(T) = \{p : p' = 0\} = \mathrm{span}\{1\} ker ( T ) = { p : p ′ = 0 } = span { 1 } So dim ( ker ( T ) ) = 1 \dim(\ker(T)) = 1 dim ( ker ( T )) = 1 .
i m ( T ) = { p ′ : p ∈ P 2 } = s p a n { 1 , x } \mathrm{im}(T) = \{p' : p \in \mathcal{P}_2\} = \mathrm{span}\{1, x\} im ( T ) = { p ′ : p ∈ P 2 } = span { 1 , x } So dim ( i m ( T ) ) = 2 \dim(\mathrm{im}(T)) = 2 dim ( im ( T )) = 2 .
Verify: dim ( ker ( T ) ) + dim ( i m ( T ) ) = 1 + 2 = 3 = dim ( P 2 ) \dim(\ker(T)) + \dim(\mathrm{im}(T)) = 1 + 2 = 3 = \dim(\mathcal{P}_2) dim ( ker ( T )) + dim ( im ( T )) = 1 + 2 = 3 = dim ( P 2 ) . ■ \blacksquare ■
If you get this wrong, revise: Section 6.2 (Matrix Representation) and Section 6.4 (Rank-Nullity).
Linear algebra is the mathematics of linearity: systems where superposition holds. The key insight is that linear transformations are completely determined by what they do to a basis, and eigenvalues tell you the scaling factors along special directions. Determinants measure volume distortion: a zero determinant means the transformation squashes space into a lower dimension, making inversion impossible. The rank-nullity theorem captures a conservation law: the dimensions consumed by the kernel plus the dimensions remaining in the image always equal the total dimension of the input space.
Confusing linear independence and span. Linear independence means no non-trivial linear combination equals zero; span is the set of all linear combinations. Fix: { v 1 , … , v n } \{v_1, \ldots, v_n\} { v 1 , … , v n } is linearly independent iff the equation ∑ c i v i = 0 \sum c_i v_i = 0 ∑ c i v i = 0 implies all c i = 0 c_i = 0 c i = 0 .Wrong determinant interpretation. det ( A ) = 0 \det(A) = 0 det ( A ) = 0 means A A A is singular (non-invertible); det ( A ) ≠ 0 \det(A) \neq 0 det ( A ) = 0 means A A A is invertible. Fix: A matrix is invertible iff its determinant is non-zero.Confusing eigenvalues and eigenvectors. An eigenvalue λ \lambda λ satisfies det ( A − λ I ) = 0 \det(A - \lambda I) = 0 det ( A − λ I ) = 0 ; eigenvectors are the non-zero solutions of ( A − λ I ) v = 0 (A - \lambda I)v = 0 ( A − λ I ) v = 0 . Fix: Find eigenvalues from the characteristic polynomial; then find eigenvectors by solving ( A − λ I ) v = 0 (A - \lambda I)v = 0 ( A − λ I ) v = 0 .Problem. Find the determinant of A = ( 1 2 3 0 1 4 5 6 0 ) A = \begin{pmatrix} 1 & 2 & 3 \\ 0 & 1 & 4 \\ 5 & 6 & 0 \end{pmatrix} A = 1 0 5 2 1 6 3 4 0 and determine if A A A is invertible.
Solution. det ( A ) = 1 ( 0 − 24 ) − 2 ( 0 − 20 ) + 3 ( 0 − 5 ) = − 24 + 40 − 15 = 1 ≠ 0 \det(A) = 1(0 - 24) - 2(0 - 20) + 3(0 - 5) = -24 + 40 - 15 = 1 \neq 0 det ( A ) = 1 ( 0 − 24 ) − 2 ( 0 − 20 ) + 3 ( 0 − 5 ) = − 24 + 40 − 15 = 1 = 0 .
Since det ( A ) ≠ 0 \det(A) \neq 0 det ( A ) = 0 , A A A is invertible. ■ \blacksquare ■
Problem. Find the eigenvalues and eigenvectors of A = ( 4 1 2 3 ) A = \begin{pmatrix} 4 & 1 \\ 2 & 3 \end{pmatrix} A = ( 4 2 1 3 ) .
Solution. det ( A − λ I ) = ( 4 − λ ) ( 3 − λ ) − 2 = λ 2 − 7 λ + 10 = ( λ − 5 ) ( λ − 2 ) = 0 \det(A - \lambda I) = (4-\lambda)(3-\lambda) - 2 = \lambda^2 - 7\lambda + 10 = (\lambda - 5)(\lambda - 2) = 0 det ( A − λ I ) = ( 4 − λ ) ( 3 − λ ) − 2 = λ 2 − 7 λ + 10 = ( λ − 5 ) ( λ − 2 ) = 0 .
Eigenvalues: λ 1 = 5 \lambda_1 = 5 λ 1 = 5 , λ 2 = 2 \lambda_2 = 2 λ 2 = 2 .
For λ 1 = 5 \lambda_1 = 5 λ 1 = 5 : ( A − 5 I ) v = 0 ⟹ ( − 1 1 2 − 2 ) v = 0 ⟹ v 1 = ( 1 1 ) (A - 5I)v = 0 \implies \begin{pmatrix} -1 & 1 \\ 2 & -2 \end{pmatrix}v = 0 \implies v_1 = \begin{pmatrix} 1 \\ 1 \end{pmatrix} ( A − 5 I ) v = 0 ⟹ ( − 1 2 1 − 2 ) v = 0 ⟹ v 1 = ( 1 1 ) .
For λ 2 = 2 \lambda_2 = 2 λ 2 = 2 : ( A − 2 I ) v = 0 ⟹ ( 2 1 2 1 ) v = 0 ⟹ v 2 = ( 1 − 2 ) (A - 2I)v = 0 \implies \begin{pmatrix} 2 & 1 \\ 2 & 1 \end{pmatrix}v = 0 \implies v_2 = \begin{pmatrix} 1 \\ -2 \end{pmatrix} ( A − 2 I ) v = 0 ⟹ ( 2 2 1 1 ) v = 0 ⟹ v 2 = ( 1 − 2 ) .
■ \blacksquare ■
A[9_Problem Set] --> B[Key Concepts]
A --> D[Practical Applications]
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D --> G[Real-world usage]
A matrix is invertible iff det ( A ) ≠ 0 \det(A) \neq 0 det ( A ) = 0 ; equivalent to having linearly independent rows/columns. Eigenvalues: roots of the characteristic polynomial det ( A − λ I ) = 0 \det(A - \lambda I) = 0 det ( A − λ I ) = 0 . Eigenvectors: non-zero vectors in ker ( A − λ I ) \ker(A - \lambda I) ker ( A − λ I ) . The spectral theorem: a real symmetric matrix has an orthonormal eigenbasis and can be diagonalised. Topic Site Link Linear Algebra (Overview) WyattsNotes View Abstract Algebra WyattsNotes View Multivariable Calculus WyattsNotes View Linear Algebra — MIT 18.06 MIT OCW View