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Linear Algebra Exercises-n-Answers.pdf

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122 <strong>Linear</strong> <strong>Algebra</strong>, by Hefferon<br />

we can either solve the<br />

(<br />

system<br />

( ) ( ) ( ) ( ) ( )<br />

1 x1 x2 0 x1 x2<br />

= 5 + 0<br />

= 0 + 4<br />

0)<br />

y 1 y 1 1 y 1 y 1<br />

or else just spot the answer (thinking of the<br />

(<br />

proof<br />

)<br />

of<br />

(<br />

Lemma<br />

)<br />

1.4).<br />

1/5 0<br />

D = 〈 , 〉<br />

0 1/4<br />

(b) Yes, this matrix is nonsingular and so changes<br />

( )<br />

bases.<br />

( )<br />

To calculate D, we proceed as above with<br />

x1 x2<br />

D = 〈 , 〉<br />

y 1 y 2<br />

to solve (<br />

1<br />

0)<br />

( ) ( )<br />

x1 x2<br />

= 2 + 3<br />

y 1 y 1<br />

and<br />

(<br />

0<br />

1)<br />

( ) ( )<br />

x1 x2<br />

= 1 + 1<br />

y 1 y 1<br />

and get this.<br />

( ) (<br />

−1 1<br />

D = 〈 , 〉<br />

3 −2)<br />

(c) No, this matrix does not change bases because it is nonsingular.<br />

(d) Yes, this matrix changes bases because it is nonsingular. The calculation of the changed-to basis<br />

is as above.<br />

( ) ( )<br />

1/2 1/2<br />

D = 〈 , 〉<br />

−1/2 1/2<br />

Three.V.1.11 This question has many different solutions. One way to proceed is to make up any basis<br />

B for any space, and then compute the appropriate D (necessarily for the same space, of course).<br />

Another, easier, way to proceed is to fix the codomain as R 3 and the codomain basis as E 3 . This way<br />

(recall that the representation of any vector with respect to the standard basis is just the vector itself),<br />

we have this.<br />

⎛<br />

B = 〈 ⎝ 3 ⎞ ⎛<br />

2⎠ , ⎝ 1<br />

⎞ ⎛<br />

−1⎠ , ⎝ 4 ⎞<br />

1⎠〉 D = E 3<br />

0 0 4<br />

Three.V.1.12 Checking that B = 〈2 sin(x) + cos(x), 3 cos(x)〉 is a basis is routine. Call the natural<br />

basis D. To compute the change of basis matrix Rep B,D (id) we must find Rep D (2 sin(x) + cos(x)) and<br />

Rep D (3 cos(x)), that is, we need x 1 , y 1 , x 2 , y 2 such that these equations hold.<br />

x 1 · sin(x) + y 1 · cos(x) = 2 sin(x) + cos(x)<br />

x 2 · sin(x) + y 2 · cos(x) = 3 cos(x)<br />

Obviously this is the answer.<br />

( )<br />

2 0<br />

Rep B,D (id) =<br />

1 3<br />

For the change of basis matrix in the other direction we could look for Rep B (sin(x)) and Rep B (cos(x))<br />

by solving these.<br />

w 1 · (2 sin(x) + cos(x)) + z 1 · (3 cos(x)) = sin(x)<br />

w 2 · (2 sin(x) + cos(x)) + z 2 · (3 cos(x)) = cos(x)<br />

An easier method is to find the inverse<br />

(<br />

of the<br />

)<br />

matrix found above.<br />

−1<br />

2 0<br />

Rep D,B (id) =<br />

= 1 ( ) ( )<br />

3 0 1/2 0<br />

1 3 6 · =<br />

−1 2 −1/6 1/3<br />

Three.V.1.13 We start by taking the inverse of the matrix, that is, by deciding what is the inverse to<br />

the map of interest.<br />

( ) ( )<br />

Rep D,E2 (id)Rep D,E2 (id) −1 1<br />

− cos(2θ) − sin(2θ) cos(2θ) sin(2θ)<br />

=<br />

− cos 2 (2θ) − sin 2 (2θ) ·<br />

=<br />

− sin(2θ) cos(2θ) sin(2θ) − cos(2θ)<br />

This is more tractable than the representation the other way because this matrix is the concatenation<br />

of these two column vectors ( )<br />

( )<br />

Rep E2<br />

( ⃗ cos(2θ)<br />

δ 1 ) =<br />

Rep<br />

sin(2θ)<br />

E2<br />

( ⃗ sin(2θ)<br />

δ 2 ) =<br />

− cos(2θ)<br />

and representations with respect to E<br />

( 2 are transparent.<br />

) ( )<br />

⃗ cos(2θ)<br />

δ1 = ⃗ sin(2θ)<br />

δ2 =<br />

sin(2θ)<br />

− cos(2θ)<br />

This pictures the action of the map that transforms D to E 2 (it is, again, the inverse of the map that<br />

is the answer to this question). The line lies at an angle θ to the x axis.

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