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Thomas Calculus 13th [Solutions]

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Section 13.4 Curvature and Normal Vectors of a Curve 949<br />

18. r a cos t i bsin t j v a sin t i b cos t j a a cos t i bsin<br />

t j<br />

i j k<br />

v a<br />

v a a sin t b cos t 0 abk v a ab ab,<br />

since a b 0; ( t)<br />

3<br />

v<br />

a cos t bsin t 0<br />

2 2 2 2<br />

3 2<br />

2 2 2 2<br />

5 2<br />

2 2<br />

ab a sin t b cos t ; ( t) 3 ab a sin t b cos t 2a sin t cos t 2b sin t cost<br />

2<br />

2 2 2 2 2 2<br />

5 2<br />

3 ab a b sin t a sin t b cos t ; thus, ( t) 0 sin 2t 0 t 0, identifying points<br />

2<br />

on the major axis, or t , 3 identifying points on the minor axis. Furthermore, ( t ) 0 for 0 t and<br />

2 2<br />

2<br />

for t 32 ; ( t ) 0 for t and 3 t 2 . Therefore, the points associated with t 0 and t<br />

2<br />

2<br />

on the major axis give absolute maximum curvature and the points associated with t and t 3 on the<br />

2<br />

2<br />

minor axis give absolute minimum curvature.<br />

19.<br />

2 2<br />

a d a b 2 2<br />

; d 0 a b 0 a b a b since a, b 0. Now, d 0<br />

2 2 da 2 2<br />

2<br />

a b da<br />

da<br />

a b<br />

if a<br />

b<br />

and d 0<br />

da<br />

if a b is at a maximum for a b and ( b ) b 1 is the maximum value of<br />

2 2<br />

b b 2b<br />

20. (a) From Example 5, the curvature of the helix r( t) a cost i asin t j btk , a, b 0 is a ; also<br />

2 2<br />

a b<br />

v a<br />

2 b<br />

2 . For the helix r( t) 3cost i 3sin t j tk , 0 t 4 , a 3 and b 1 3 3<br />

2 2<br />

3 1 10<br />

4<br />

4<br />

and v 10 K 3 10 dt 3 t 12<br />

0 10<br />

10 0 10<br />

2<br />

2 2 2<br />

(b) y x x t and y t , t r( t) ti t j v i 2t j v 1 4 t ;<br />

2<br />

1 2t d T<br />

; 4t 2 d T<br />

T i j i j ; 16t<br />

4 2 . Thus 1 2t<br />

2 2 2<br />

3 2<br />

2<br />

3 2<br />

2<br />

3 2<br />

1 4t 1 4t dt dt 2<br />

1 4t 1 4t 1 4t<br />

1 4t<br />

2<br />

1 4t<br />

1 4t<br />

2<br />

1 4t<br />

2<br />

3<br />

.<br />

2 2<br />

2<br />

0<br />

K 1 4t dt dt lim 2 dt lim b 2 dt<br />

1 4t<br />

a<br />

b<br />

Then<br />

3 2 2 2<br />

2<br />

1 4t a 1 4t 0 1 4t<br />

1<br />

0<br />

1 1 1<br />

lim tan 2t lim tan 2t b<br />

lim tan 2a lim tan 2b<br />

a a b 0 a b<br />

2 2<br />

21.<br />

2 2<br />

2 2<br />

r ti sin t j v i cost j v 1 cost 1 cos t v 1 cos 1;<br />

2 2<br />

i cost j d T sin<br />

sin<br />

sin t cost sin t d T t d T<br />

T v<br />

i j ; 1 1. Thus<br />

v 1 cos<br />

1<br />

1 cos 1 cos<br />

2<br />

2 2<br />

3 2<br />

2<br />

3 2 2 2<br />

t<br />

dt dt 1 cos dt<br />

t t<br />

t t 1 cos<br />

2<br />

2<br />

1 1 1 1 1 and the center is<br />

2 1 1<br />

2<br />

2<br />

,0 x y 1<br />

2 2<br />

22.<br />

2 2 2<br />

r 2ln t i t 1 j v 2 i 1 1 j v 4 1 1 t 1 T v 2 t i t 1 j;<br />

t t 2 2 2 2 2 2<br />

t t t t v t 1 t 1<br />

2 2<br />

2<br />

2<br />

d T 2 t 1 4 t 1 16t<br />

4t<br />

d T<br />

i j 2 . Thus<br />

dt 2<br />

2<br />

2<br />

2 dt 2<br />

4 2<br />

t 1 t 1 t 1 t 1<br />

v<br />

d T 2 2<br />

t 2 2t<br />

dt t 1 t 1 t 1<br />

2 2<br />

2<br />

2<br />

Copyright<br />

2014 Pearson Education, Inc.

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