Linear Algebra Exercises-n-Answers.pdf

Linear Algebra Exercises-n-Answers.pdf Linear Algebra Exercises-n-Answers.pdf

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106 Linear Algebra, by Hefferon Three.III.2.17 Yes. Consider H = ( ) 1 0 0 1 representing a map from R 2 to R 2 . With respect to the standard bases B 1 = E 2 , D 1 = E 2 this matrix represents the identity map. With respect to ( ( ) 1 1 B 2 = D 2 = 〈 , 〉 1) −1 this matrix again represents the identity. In fact, as long as the starting and ending bases are equal — as long as B i = D i — then the map represented by H is the identity. Three.III.2.18 This is immediate from Corollary 2.6. Three.III.2.19 The first map ( ( x x = y) y) E 2 ↦→ ( ) 3x 2y E 2 = ( ) 3x 2y stretches vectors by a factor of three in the x direction and by a factor of two in the y direction. The second map ( ( ( ( x x x x = ↦→ y) y) 0) 0) projects vectors onto the x axis. The third ( ( x x = y) y) E 2 E 2 E 2 ( y ↦→ x) interchanges first and second components (that is, it is a reflection about the line y = x). The last ( ( ( ) ( ) x x x + 3y x + 3y = ↦→ y) y) y y stretches vectors parallel to the y axis, by an amount equal to three times their distance from that axis (this is a skew.) Three.III.2.20 (a) This is immediate from Theorem 2.3. (b) Yes. This is immediate from the prior item. To give a specific example, we can start with E 3 as the basis for the domain, and then we require a basis D for the codomain R 3 . The matrix H gives the action of the map as this ⎛ ⎞ ⎛ ⎞ ⎛ ⎞ ⎛ ⎞ ⎛ ⎞ ⎛ ⎞ ⎛ ⎞ ⎛ ⎞ ⎛ ⎞ ⎝ 1 0⎠ = 0 ⎝ 1 0 0 ⎠E 3 ↦→ ⎝ 1 2⎠ 0 D ⎝ 0 1⎠ = 0 ⎝ 0 1 0 and there is no harm in finding a basis D so that ⎛ ⎞ ⎛ ⎞ Rep D ( ⎝ 1 0⎠) = ⎝ 1 2⎠ 0 0 D ⎠E 3 ↦→ E 2 = E 2 = E 2 = ⎝ 0 0⎠ 1 ( y x) D ⎛ ⎞ ⎝ 0 0⎠ = 1 ⎛ ⎝ 0 0 1 ⎞ and Rep D ( ⎝ 0 1⎠) = ⎝ 0 0⎠ 0 1 D ⎠E 3 ↦→ ⎝ 0 0⎠ 0 that is, so that the map represented by H with respect to E 3 , D is projection down onto the xy plane. The second condition gives that the third member of D is ⃗e 2 . The first condition gives that the first member of D plus twice the second equals ⃗e 1 , and so this basis will do. ⎛ D = 〈 ⎝ 0 ⎞ ⎛ −1⎠ , ⎝ 1/2 ⎞ ⎛ 1/2⎠ , ⎝ 0 ⎞ 1⎠〉 0 0 0 Three.III.2.21 (a) Recall that the representation map Rep B : V → R n is linear (it is actually an isomorphism, but we do not need that it is one-to-one or onto here). Considering the column vector x to be a n×1 matrix gives that the map from R n to R that takes a column vector to its dot product with ⃗x is linear (this is a matrix-vector product and so Theorem 2.1 applies). Thus the map under consideration h ⃗x is linear because it is the composistion of two linear maps. ⃗v ↦→ Rep B (⃗v) ↦→ ⃗x · Rep B (⃗v) (b) Any linear map g : V → R is represented by some matrix ( g1 g 2 · · · g n ) D

Answers to Exercises 107 (the matrix has n columns because V is n-dimensional and it has only one row because R is onedimensional). Then taking ⃗x to be the column vector that is the transpose of this matrix ⎛ ⎞ g 1 ⎜ ⃗x = . ⎟ ⎝ . ⎠ g n has the desired action. ⎛ ⎞ ⎛ ⎞ ⎛ ⎞ v 1 g 1 v 1 ⎜ ⃗v = . ⎟ ⎜ ⎝ . ⎠ ↦→ . ⎟ ⎜ . ⎟ ⎝ . ⎠ ⎝ . ⎠ = g 1 v 1 + · · · + g n v n v n g n v n (c) No. If ⃗x has any nonzero entries then h ⃗x cannot be the zero map (and if ⃗x is the zero vector then h ⃗x can only be the zero map). Three.III.2.22 See the following section. Subsection Three.IV.1: Sums and Scalar Products Three.IV.1.7 (a) (e) Not defined. ( 7 0 ) 6 9 1 6 (b) ( 12 −6 ) −6 6 12 18 (c) ( ) 4 2 0 6 (d) ( ) −1 28 2 1 Three.IV.1.8 Represent the domain vector ⃗v ∈ V and the maps g, h: V → W with respect to bases B, D in the usual way. (a) The representation of (g + h) (⃗v) = g(⃗v) + h(⃗v) ( (g1,1 v 1 + · · · + g 1,n v n ) ⃗ δ 1 + · · · + (g m,1 v 1 + · · · + g m,n v n ) ⃗ ) δ m regroups + ( (h 1,1 v 1 + · · · + h 1,n v n ) ⃗ δ 1 + · · · + (h m,1 v 1 + · · · + h m,n v n ) ⃗ δ m ) = ((g 1,1 + h 1,1 )v 1 + · · · + (g 1,1 + h 1,n )v n ) · ⃗δ 1 + · · · + ((g m,1 + h m,1 )v 1 + · · · + (g m,n + h m,n )v n ) · ⃗δ m to the entry-by-entry sum of the representation of g(⃗v) and the representation of h(⃗v). (b) The representation of (r · h) (⃗v) = r · (h(⃗v) ) r · ((h 1,1 v 1 + h 1,2 v 2 + · · · + h 1,n v n ) ⃗ δ 1 + · · · + (h m,1 v 1 + h m,2 v 2 + · · · + h m,n v n ) ⃗ δ m ) = (rh 1,1 v 1 + · · · + rh 1,n v n ) · ⃗δ 1 + · · · + (rh m,1 v 1 + · · · + rh m,n v n ) · ⃗δ m is the entry-by-entry multiple of r and the representation of h. Three.IV.1.9 First, each of these properties is easy to check in an entry-by-entry way. For example, writing ⎛ ⎞ ⎛ ⎞ g 1,1 . . . g 1,n h 1,1 . . . h 1,n ⎜ ⎟ ⎜ ⎟ G = ⎝ . . ⎠ H = ⎝ . . ⎠ g m,1 . . . g m,n h m,1 . . . h m,n then, by definition we have ⎛ ⎞ ⎛ ⎞ g 1,1 + h 1,1 . . . g 1,n + h 1,n h 1,1 + g 1,1 . . . h 1,n + g 1,n ⎜ G + H = . . ⎟ ⎜ ⎝ . . ⎠ H + G = . . ⎟ ⎝ . . ⎠ g m,1 + h m,1 . . . g m,n + h m,n h m,1 + g m,1 . . . h m,n + g m,n and the two are equal since their entries are equal g i,j + h i,j = h i,j + g i,j . That is, each of these is easy to check by using Definition 1.3 alone. However, each property is also easy to understand in terms of the represented maps, by applying Theorem 1.5 as well as the definition. (a) The two maps g + h and h + g are equal because g(⃗v) + h(⃗v) = h(⃗v) + g(⃗v), as addition is commutative in any vector space. Because the maps are the same, they must have the same representative. (b) As with the prior answer, except that here we apply that vector space addition is associative. (c) As before, except that here we note that g(⃗v) + z(⃗v) = g(⃗v) + ⃗0 = g(⃗v). (d) Apply that 0 · g(⃗v) = ⃗0 = z(⃗v).

<strong>Answers</strong> to <strong>Exercises</strong> 107<br />

(the matrix has n columns because V is n-dimensional and it has only one row because R is onedimensional).<br />

Then taking ⃗x to be the column vector that is the transpose of this matrix<br />

⎛ ⎞<br />

g 1<br />

⎜<br />

⃗x = . ⎟<br />

⎝ . ⎠<br />

g n<br />

has the desired action.<br />

⎛ ⎞ ⎛ ⎞ ⎛ ⎞<br />

v 1 g 1 v 1<br />

⎜<br />

⃗v = . ⎟ ⎜<br />

⎝ . ⎠ ↦→ . ⎟ ⎜ . ⎟<br />

⎝ . ⎠ ⎝ . ⎠ = g 1 v 1 + · · · + g n v n<br />

v n g n v n<br />

(c) No. If ⃗x has any nonzero entries then h ⃗x cannot be the zero map (and if ⃗x is the zero vector then<br />

h ⃗x can only be the zero map).<br />

Three.III.2.22<br />

See the following section.<br />

Subsection Three.IV.1: Sums and Scalar Products<br />

Three.IV.1.7<br />

(a)<br />

(e) Not defined.<br />

( 7 0<br />

) 6<br />

9 1 6<br />

(b)<br />

( 12 −6<br />

) −6<br />

6 12 18<br />

(c)<br />

( ) 4 2<br />

0 6<br />

(d)<br />

( ) −1 28<br />

2 1<br />

Three.IV.1.8 Represent the domain vector ⃗v ∈ V and the maps g, h: V → W with respect to bases<br />

B, D in the usual way.<br />

(a) The representation of (g + h) (⃗v) = g(⃗v) + h(⃗v)<br />

(<br />

(g1,1 v 1 + · · · + g 1,n v n ) ⃗ δ 1 + · · · + (g m,1 v 1 + · · · + g m,n v n ) ⃗ )<br />

δ m<br />

regroups<br />

+ ( (h 1,1 v 1 + · · · + h 1,n v n ) ⃗ δ 1 + · · · + (h m,1 v 1 + · · · + h m,n v n ) ⃗ δ m<br />

)<br />

= ((g 1,1 + h 1,1 )v 1 + · · · + (g 1,1 + h 1,n )v n ) · ⃗δ 1 + · · · + ((g m,1 + h m,1 )v 1 + · · · + (g m,n + h m,n )v n ) · ⃗δ m<br />

to the entry-by-entry sum of the representation of g(⃗v) and the representation of h(⃗v).<br />

(b) The representation of (r · h) (⃗v) = r · (h(⃗v) )<br />

r · ((h<br />

1,1 v 1 + h 1,2 v 2 + · · · + h 1,n v n ) ⃗ δ 1 + · · · + (h m,1 v 1 + h m,2 v 2 + · · · + h m,n v n ) ⃗ δ m<br />

)<br />

= (rh 1,1 v 1 + · · · + rh 1,n v n ) · ⃗δ 1 + · · · + (rh m,1 v 1 + · · · + rh m,n v n ) · ⃗δ m<br />

is the entry-by-entry multiple of r and the representation of h.<br />

Three.IV.1.9 First, each of these properties is easy to check in an entry-by-entry way. For example,<br />

writing<br />

⎛<br />

⎞ ⎛<br />

⎞<br />

g 1,1 . . . g 1,n<br />

h 1,1 . . . h 1,n<br />

⎜<br />

⎟ ⎜<br />

⎟<br />

G = ⎝ . . ⎠ H = ⎝ . . ⎠<br />

g m,1 . . . g m,n h m,1 . . . h m,n<br />

then, by definition we have<br />

⎛<br />

⎞<br />

⎛<br />

⎞<br />

g 1,1 + h 1,1 . . . g 1,n + h 1,n<br />

h 1,1 + g 1,1 . . . h 1,n + g 1,n<br />

⎜<br />

G + H =<br />

.<br />

. ⎟<br />

⎜<br />

⎝ .<br />

. ⎠ H + G =<br />

.<br />

. ⎟<br />

⎝ .<br />

. ⎠<br />

g m,1 + h m,1 . . . g m,n + h m,n h m,1 + g m,1 . . . h m,n + g m,n<br />

and the two are equal since their entries are equal g i,j + h i,j = h i,j + g i,j . That is, each of these is easy<br />

to check by using Definition 1.3 alone.<br />

However, each property is also easy to understand in terms of the represented maps, by applying<br />

Theorem 1.5 as well as the definition.<br />

(a) The two maps g + h and h + g are equal because g(⃗v) + h(⃗v) = h(⃗v) + g(⃗v), as addition is commutative<br />

in any vector space. Because the maps are the same, they must have the same representative.<br />

(b) As with the prior answer, except that here we apply that vector space addition is associative.<br />

(c) As before, except that here we note that g(⃗v) + z(⃗v) = g(⃗v) + ⃗0 = g(⃗v).<br />

(d) Apply that 0 · g(⃗v) = ⃗0 = z(⃗v).

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