Linear Algebra Exercises-n-Answers.pdf

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

math.hcmuns.edu.vn
from math.hcmuns.edu.vn More from this publisher
11.04.2014 Views

118 Linear Algebra, by Hefferon As a check, note that the third column of the starting matrix is 3/2 times the second, and so it is indeed singular and therefore has no inverse. Three.IV.4.17 We can use Corollary 4.12. 1 1 · 5 − 2 · 3 · ( ) ( ) 5 −3 −5 3 = −2 1 2 −1 Three.IV.4.18 (a) The proof that the inverse is r −1 H −1 = (1/r) · H −1 (provided, of course, that the matrix is invertible) is easy. (b) No. For one thing, the fact that H + G has an inverse doesn’t imply that H has an inverse or that G has an inverse. Neither of these matrices is invertible but their sum is. ( ) ( ) 1 0 0 0 0 0 0 1 Another point is that just because H and G each has an inverse doesn’t mean H + G has an inverse; here is an example. ( ) ( ) 1 0 −1 0 0 1 0 −1 Still a third point is that, even if the two matrices have inverses, and the sum has an inverse, doesn’t imply that the equation holds: ( ) −1 ( ) −1 ( ) −1 ( ) −1 2 0 1/2 0 3 0 1/3 0 = = 0 2 0 1/2 0 3 0 1/3 but and (1/2) + (1/3) does not equal 1/5. ( ) −1 ( ) −1 5 0 1/5 0 = 0 5 0 1/5 Three.IV.4.19 Yes: T k (T −1 ) k = (T T · · · T ) · (T −1 T −1 · · · T −1 ) = T k−1 (T T −1 )(T −1 ) k−1 = · · · = I. Three.IV.4.20 Yes, the inverse of H −1 is H. Three.IV.4.21 One way to check that the first is true is with the angle sum formulas from trigonometry. (cos(θ1 ) ( ) + θ 2 ) − sin(θ 1 + θ 2 ) cos θ1 cos θ = 2 − sin θ 1 sin θ 2 − sin θ 1 cos θ 2 − cos θ 1 sin θ 2 sin(θ 1 + θ 2 ) cos(θ 1 + θ 2 ) sin θ 1 cos θ 2 + cos θ 1 sin θ 2 cos θ 1 cos θ 2 − sin θ 1 sin θ 2 ( ) ( ) cos θ1 − sin θ = 1 cos θ2 − sin θ 2 sin θ 1 cos θ 1 sin θ 2 cos θ 2 Checking the second equation in this way is similar. Of course, the equations can be not just checked but also understood by recalling that t θ is the map that rotates vectors about the origin through an angle of θ radians. Three.IV.4.22 There are two cases. For the first case we assume that a is nonzero. Then ( ) ( ) −(c/a)ρ 1 +ρ 2 a b 1 0 a b 1 0 −→ = 0 −(bc/a) + d −c/a 1 0 (ad − bc)/a −c/a 1 shows that the matrix is invertible (in this a ≠ 0 case) if and only if ad − bc ≠ 0. To find the inverse, we finish with the Jordan half of the reduction. ( ) ( ) (1/a)ρ 1 1 b/a 1/a 0 −(b/a)ρ 2+ρ 1 1 0 d/(ad − bc) −b/(ad − bc) −→ −→ (a/ad−bc)ρ 2 0 1 −c/(ad − bc) a/(ad − bc) 0 1 −c/(ad − bc) a/(ad − bc) The other case is the a = 0 case. We swap to get c into the 1, 1 position. ( ) ρ 1↔ρ 2 c d 0 1 −→ 0 b 1 0 This matrix is nonsingular if and only if both b and c are nonzero (which, under the case assumption that a = 0, holds if and only if ad − bc ≠ 0). To find the inverse we do the Jordan half. ( ) ( ) (1/c)ρ 1 1 d/c 0 1/c −(d/c)ρ 2+ρ 1 1 0 −d/bc 1/c −→ −→ (1/b)ρ 2 0 1 1/b 0 0 1 1/b 0 (Note that this is what is required, since a = 0 gives that ad − bc = −bc).

Answers to Exercises 119 Three.IV.4.23 With H a 2×3 matrix, in looking for a matrix G such that the combination HG acts as the 2×2 identity we need G to be 3×2. Setting up the equation ( ) ⎛ 1 0 1 ⎝ m n ⎞ ( ) p q⎠ 1 0 = 0 1 0 0 1 r s and solving the resulting linear system m +r = 1 n +s = 0 p = 0 q = 1 gives infinitely many solutions. ⎛ ⎞ ⎛ ⎞ ⎛ ⎞ ⎛ ⎞ m 1 −1 0 n 0 0 −1 { p ⎜ q = 0 ⎟ ⎜1 + r · 0 ⎟ ⎜ 0 + s · 0 ∣ ⎟ ⎜ 0 r, s ∈ R} ⎟ ⎝ r ⎠ ⎝0⎠ ⎝ 1 ⎠ ⎝ 0 ⎠ s 0 0 1 Thus H has infinitely many right inverses. As for left inverses, the equation ⎛ ( ) ( ) a b 1 0 1 = ⎝ 1 0 0 ⎞ 0 1 0⎠ c d 0 1 0 0 0 1 gives rise to a linear system with nine equations and four unknowns. a = 1 b = 0 a = 0 c = 0 d = 1 c = 0 e = 0 f = 0 e = 1 This system is inconsistent (the first equation conflicts with the third, as do the seventh and ninth) and so there is no left inverse. Three.IV.4.24 With respect to the standard bases we have ⎛ Rep E2 ,E 3 (η) = ⎝ 1 0 ⎞ 0 1⎠ 0 0 and setting up the equation to find the matrix inverse ( ) ⎛ a b c ⎝ 1 0 ⎞ ( ) 0 1⎠ 1 0 = = Rep d e f 0 1 E2 ,E 2 (id) 0 0 gives rise to a linear system. a = 1 b = 0 d = 0 e = 1 There are infinitely many solutions in a, . . . , f to this system because two of these variables are entirely unrestricted ⎛ ⎞ ⎛ ⎞ ⎛ ⎞ ⎛ ⎞ a 1 0 0 b 0 0 0 { c ⎜d = 0 ⎟ ⎜0 + c · 1 ⎟ ⎜0 + f · 0 ∣ ⎟ ⎜0 c, f ∈ R} ⎟ ⎝e⎠ ⎝1⎠ ⎝0⎠ ⎝0⎠ f 0 0 1

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

As a check, note that the third column of the starting matrix is 3/2 times the second, and so it is<br />

indeed singular and therefore has no inverse.<br />

Three.IV.4.17 We can use Corollary 4.12.<br />

1<br />

1 · 5 − 2 · 3 ·<br />

( ) ( )<br />

5 −3 −5 3<br />

=<br />

−2 1 2 −1<br />

Three.IV.4.18 (a) The proof that the inverse is r −1 H −1 = (1/r) · H −1 (provided, of course, that<br />

the matrix is invertible) is easy.<br />

(b) No. For one thing, the fact that H + G has an inverse doesn’t imply that H has an inverse or<br />

that G has an inverse. Neither of these matrices is invertible but their sum is.<br />

( ) ( )<br />

1 0 0 0<br />

0 0 0 1<br />

Another point is that just because H and G each has an inverse doesn’t mean H + G has an inverse;<br />

here is an example.<br />

( ) ( )<br />

1 0 −1 0<br />

0 1 0 −1<br />

Still a third point is that, even if the two matrices have inverses, and the sum has an inverse, doesn’t<br />

imply that the equation holds:<br />

( ) −1 ( ) −1 ( ) −1 ( ) −1<br />

2 0 1/2 0<br />

3 0 1/3 0<br />

=<br />

=<br />

0 2 0 1/2 0 3 0 1/3<br />

but<br />

and (1/2) + (1/3) does not equal 1/5.<br />

( ) −1 ( ) −1<br />

5 0 1/5 0<br />

=<br />

0 5 0 1/5<br />

Three.IV.4.19 Yes: T k (T −1 ) k = (T T · · · T ) · (T −1 T −1 · · · T −1 ) = T k−1 (T T −1 )(T −1 ) k−1 = · · · = I.<br />

Three.IV.4.20 Yes, the inverse of H −1 is H.<br />

Three.IV.4.21 One way to check that the first is true is with the angle sum formulas from trigonometry.<br />

(cos(θ1 ) ( )<br />

+ θ 2 ) − sin(θ 1 + θ 2 ) cos θ1 cos θ<br />

=<br />

2 − sin θ 1 sin θ 2 − sin θ 1 cos θ 2 − cos θ 1 sin θ 2<br />

sin(θ 1 + θ 2 ) cos(θ 1 + θ 2 ) sin θ 1 cos θ 2 + cos θ 1 sin θ 2 cos θ 1 cos θ 2 − sin θ 1 sin θ 2<br />

( ) ( )<br />

cos θ1 − sin θ<br />

=<br />

1 cos θ2 − sin θ 2<br />

sin θ 1 cos θ 1 sin θ 2 cos θ 2<br />

Checking the second equation in this way is similar.<br />

Of course, the equations can be not just checked but also understood by recalling that t θ is the<br />

map that rotates vectors about the origin through an angle of θ radians.<br />

Three.IV.4.22<br />

There are two cases. For the first case we assume that a is nonzero. Then<br />

( ) ( )<br />

−(c/a)ρ 1 +ρ 2 a b 1 0 a b 1 0<br />

−→ =<br />

0 −(bc/a) + d −c/a 1 0 (ad − bc)/a −c/a 1<br />

shows that the matrix is invertible (in this a ≠ 0 case) if and only if ad − bc ≠ 0. To find the inverse,<br />

we finish with the Jordan half of the reduction.<br />

( )<br />

( )<br />

(1/a)ρ 1 1 b/a 1/a 0 −(b/a)ρ 2+ρ 1 1 0 d/(ad − bc) −b/(ad − bc)<br />

−→<br />

−→<br />

(a/ad−bc)ρ 2<br />

0 1 −c/(ad − bc) a/(ad − bc)<br />

0 1 −c/(ad − bc) a/(ad − bc)<br />

The other case is the a = 0 case. We swap to get c into the 1, 1 position.<br />

( )<br />

ρ 1↔ρ 2 c d 0 1<br />

−→<br />

0 b 1 0<br />

This matrix is nonsingular if and only if both b and c are nonzero (which, under the case assumption<br />

that a = 0, holds if and only if ad − bc ≠ 0). To find the inverse we do the Jordan half.<br />

( )<br />

( )<br />

(1/c)ρ 1 1 d/c 0 1/c −(d/c)ρ 2+ρ 1 1 0 −d/bc 1/c<br />

−→<br />

−→<br />

(1/b)ρ 2<br />

0 1 1/b 0<br />

0 1 1/b 0<br />

(Note that this is what is required, since a = 0 gives that ad − bc = −bc).

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!