cpm calculus chapter 08 solutions
DESCRIPTION
SolutionsTRANSCRIPT
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Chapter 8 Solutions Calculus
Chapter 8 Solutions 1. a. A thin cylinder. b. Answers vary. c. It should be a semicircle. 2. a. The thickness times the area gives the volume of each slice if they are modeled as
cylinders, and the summation notations add up the volumes of n slices.
b. By integration: A(x)dxL
R
! , from the left side of the line to the right, where A(x) is the area of each cross-sections, which takes the limit of estimates with smaller and smaller slices.
3. a. ! 11.8
2( )
2
+ 14.32
( )2
+ 16.52
( )2
+ 182
( )2
+ 192
( )2
+ 18.12
( )2
+ 15.32
( )2
+ 112
( )2
+ 8.42
( )2
+ 72
( )2( ) " 5
# 8259.404cm3
b. It would be more accurate. c. Integrate the areas, which takes the limit of using thinner and thinner sections of the
vase. 4. a. dx represents an infinitesimal change in x. b. It represents the area of an infinitesimally thin rectangle. 5. See graph at right. a. height = x , width = !x = i
n(9 " 5)
in a Riemann sum or dx in an integral.
b. x dx = x3 232
4
9
!9
4=23(27 " 8) = 38
3
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Chapter 8 Solutions Calculus
6. a. = 13(5x2 !17x)!2 3(10x !17)
b. = (12x2 + 2)(8 ! 7x3) + (4x3 + 2x2 ! 5)(!21x2 )= 96x2 ! 84x5 +16 !14x3 ! 84x5 ! 42x3 +105x2
= !168x5 ! 56x3 + 201x2 +16
c. = cos(sin t) !cos t d. ln(cos2 x) sin x ! 7 ln(49x2 ) 7. = ! (4x4 " 8x2 + 4 " (x4 " 2x2 +1))dx
"1
1
# = ! (3x4 " 6x2 + 3)dx"11
#
= ! ( 35x5 " 2x3 + 3x)
1
"1= ! 1 3
5" ("1 3
5)( ) = 16!5
8. a. = e3x sin(5x) + C b. = 1
4e4x+2
3
5=1
4e22!1
4e14
c. = sec x tan xdx!1 =" sec x + C d. U = sin2 x, dU = 2 sin x cos xdx = sin(2x)dx; sin(2x)2sin2x dx!
= 2U dU = 11n2
2U + C =! 11n2 "2sin2x
+ C
e. = (16x3 !16x2 + 4x)dx = 4x4 ! 163x3+ 2x2
2
0=
0
2
" 4 #16 ! 163 #8 + 8 = 72 !1283
= 29 13
9. a. 250 !1.1211 = $869.64 b. 1
11250 !1.12x dx
0
11
" = 111 !250 !1
1n1.12!1.12x
11
0=250(1.1211#1)11 ln 1.12
$ $497.06 10. a. At x = 2 there is a hole. b. At x = !4 and 1 there is no limit, and at x = 2 g is undefined. c. At x = !4,1 , and 2, because it is not continuous, and at x = !2 there is a cusp. 11. a. 3 b. 2 c. 2 d. Does not exist.
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Chapter 8 Solutions Calculus
12. a. !x by f (x) = x b. The slice is a thin cylinder with depth !x and radius f (x) , and its volume is
V = !x "# f (x)2 = !x "# ( x )2 .
c. dx !" f (x)2 =0
8
# " ( x )2dx08
# = " ! xdx08
# = " x2
2
8
0= 32"
13. a. Again, each slice is a thin cylinder, with thickness !x (or dx). b. !x "# f (c)2
c. ! f (x)2dxa
b
" 14. See graph at right. a. A slice should be a disk with radius x2 and width !x .
b. ! (x2 )2dx = ! x4dx0
3
" =!03
" ! x5
5
3
0= ! 3
5
5=2435
! 15. ! ( 6 " x )2
2
5
# dx!+!! (x " 4)258
# dx =!! (6 " x)25
# dx!+!! (x2 " 8x +16)58
# dx =
! 6x " 12x2( ) 5
2+ ! 1
3x3 " 4x2 +16x( ) 8
5== 28.5! $ 89.54 !units3
16. See graph at right. a. See sketch at right. Radius = x; x2 = y or x = y
b. ! y( )0
4
"2
dy = ! x( )0
4
"2
dx = ! x0
4
" dx = 12 ! x24
0= ! (8 # 0) = 8! !un3
17. a. ! 1
2x3 + 3( )
2
0
2
" dx b. ! 2y " 63( )2
dy3
7
#
x
y
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Chapter 8 Solutions Calculus
18. a. U = 6x4 ! 3x, dU = 24x3 ! 3 :8x3!1
6x4 !3xdx =
13
(24x3!3)dx
6x4 !3x=
13dU
U""" =13ln U + C = 1
3ln 6x4 ! 3x + C
b. = ! (x+1)33
" 9x#$%&'(5
2= ! 216
3" 45( ) " ! 273 "18( ) = 27! " ("9)! = 36!
c. = 5 ! x22
" 2x + 5 ln x + 3 + C
d. U = 11x2 ! 3,!dU = 22xdx : 2" x sin(11x2 ! 3)dx = 111 sin(11x2 ! 3) ! 22xdx"=111
sinU dU = ! 111cosU + C = ! 1
11cos(11x2 ! 3) + C"
e. U = x + 2, x =U ! 2, dU = dx :2xx+2
dx =!1
0
"2(U!2)U
du =!1
0
" 2 ! 4U( ) du = 2U ! 4 ln U!10
"0
!1
= 2(x + 2) ! 4 ln x + 20
!1= (4 ! 4 ln 2) ! (2 ! 4 ln1) = 2 ! 4 ln 2
f. U = 3x, dU = 3dx : 31!9x2
dx =du
1!U2= sin!1" U + C =" sin!1(3x) + C
19. It will look like a cone with a ridge. See diagram at right. 20. a. = lim
x!2( 12"x
+x"12"x) = lim
x!2
1+(x"1)
2"x= limx!2
x
2"x Does not exist.
b. = 018!18+1
=0
1= 0
c. = !"
d. limx!4
(2" x )
2" x= limx!4
2 + x = 2 + 2 = 4
e. limx!
1"5
x2+8
x3
24
x2+54
x3
= #
f. = limx!2
(x"2)(2x"1)
(x"2)(5x+3)= limx!2
2x"15x+3
=313
21. !R2 " ! r2 22. B: The middle integral computes a different area, but I and III compute the area of the same
region.
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Chapter 8 Solutions Calculus
23. C. If you take the derivatives of I and II you get (ln x)3x
. 24. a. 10 inches b. 0.5 inches c. ! (radius)2(thickness) " ! (radius of hole)2(thickness) d. ! (10 " 0.5i)2 (2) " ! (0.5)2(2)
e. ! 10 " 0.5i( )2 " ! 0.5( )2( )i=0
9
# $2 = 2! 10 " 0.5( )2" 0.25( )
i=0
9
#
!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!or 2! 5 + 0.5i( )2" 0.25( )
i=1
10
#
f. 1237.5! = 3887.721!in.3 25. a. A cylinder with a cone cut our of it: V = 4 !" ! 42 # 1
3! 4 !" ! 42 = 64" #
64
3" =
128"
3un3
b. ! x ! ("R2 # " r2 ) where R is the bigger radius and r is the smaller radius: ! x ! (" ! 42 # " ! x2 ) = ! x(16" # x2" )
c. (16! " x2! )dx = 16! x " x33!4
0= 64! " 64
3! = 128!
30
4
# un3 26. a. See graph above right. ! (" y + 3)2
0
4
# dy " ! (y " 3)234
# dy
b. See graph below right. ! (x + 3)2
0
1
" dx + ! (x # 3)413
" dx 27. a. They will be washers. The shape is egg-
like with a spherical hole. They are perpendicular to the x-axis.
b. ! x ! (" (#2x2 + 2)2 # " (#x2 +1)2 )
c. (! ("2x2 + 2)2 " ! ("x2 +1)2"1
1
# )dx
d. 2 (! ("2x2 + 2)2 " ! ("x2 +1)2 )0
1
# dx
x
y
x
y
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Chapter 8 Solutions Calculus
28. a. Vertical rectangles: A = ( x ! (!x))dx = x
3 2
32
1
4
" + x2
2
4
1= 8
3 2+8( ) ! 23 + 12( ) = 163 + 243 ! 76 = 806 ! 76 = 736 un2
b. Horizontal rectangles. Intersections are (0, 2) and (3, 1):
A = ((!y2 + 4
!1
2
" ) ! (2 ! y))dy = (!y2 + y + 2)dy = !y3
3+y2
2+ 2y
2
!1!1
2
"
= !83+ 2 + 4 ! 1
3+ 12! 2( ) = 103 ! !
76( ) =
206+ 76! 276= 92= 4.5 un2
29. y = 3 1! x2
4 and x goes from 2 to 2: A = 2 ! 3 1" x2
4"2
2
# dx = 3"22
# 4 " x2dx $ 18.850 un2 or 6! using a calculator or noticing that it is a semicircle.
30. y = 3 1! x2
4: the horizontal cross-sections are disks with radius 3 1! x2
4 so
V = !"2
2
# 3 1" x2
4
$%&
'()2
dx = 9! x " 9!4
* x3
4x3
2
"2"2
2
#= (18! " 6! ) " ("18! + 6! ) = 12! " ("12! ) = 24! un3
31. a. lim
x!3
x2"x"6x"3
= limx!3
(x"3)(x+2)
x"3= limx!3
(x + 2) = 5 , so f (3) must be 5, h = 5 .
b. Except h = 1 does not work, notice we squared the original equation, which left room for !3+ h and 3+ h to be opposites, so h = 6 .
c. a: When graphed, the function looks like the line x + 2. h = 5, fills in the hole at
(3, 5). Therefore the function is differentiable for all x. b: !f ( x + 6) = 1
2 x+6=
1
2 3+6=16
at x = 3. !f ("x + 6) = "1 at x = 3. Therefore the function is not differentiable at x = 3.
!3+ h = 3+ h
(!3+ h)2 = 3+ h
9 ! 6h + h2 = 3+ h
h2! 7h + 6 = 0
(h ! 6)(h !1) = 0!!"!!h = 1 or 6
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Chapter 8 Solutions Calculus
32. a. Use the reverse Chain Rule. U = ex , dU = exdx : ex(2!ex )20
1
" dx = dU(2!U )21
x=0x=0
1
"
=1
2!ex
1
0=
12!e
! 12!1
=12!e
!1 =1!(2!e)2!e
=e!12!e
b. Use the Chain Rule with g(x) = f (x)dx4
x
! and h(x) = x2 :
ddx
f (x)dx = h1(x) ! g1(h(x)) = 2x ! f (x2 )4
x2
"
c. U = sec x, dU = sec x tan xdx : sec x tan x1+sec2 x! dx =
dU
1+U2! = tan"1U + C = tan"1(sec x) + C
d. U = x2, dU = 2xdx : x1!x4
" = 12" #2xdx
1!x4=12
dU
1!U2" = 12 sin!1U + C =
12sin!1(x2 ) + C
e. = sin x 2cos x 2
dx,0
!2" U # cos x2 , dU = #
12sin( x
2)dx :
sin x 2
cos x 20
!2" dx = #2dUUx=0
!2"
= #2 ln U! /2
x=0= #2 ln(cos x
2)
! /2
x=0= #2 ln(cos !
4) + 2 ln(cos 0)
= #2 ln( 22) + 0 = #2 ln(2#1 2 ) = (# 1
2) $ (#2) ln 2 = ln 2 % 0.693
33. !f (x) = (x"3)("1)"(1)(1"x)
(x"3)2=3"x"1+x
(x"3)2=
2
(x"3)2, f 11(x) = "2 # 2
(x"3)3=
"4
(x"3)3, which is positive
when x < 3 : in (!", 3) . 34. Intersections are when
3 = x = 25 ! y2 , 9 = 25 ! y2, y2 = 16, y = 4; (3, 4)
V = (" ( 25 ! y2 )2 ! " (3)2 )dy!4
4
# = " (25 ! y2 ! 9)dy!44
# = " (16 ! y2 )dy!44
#
35. Yes (Rolles Theorem) or !f (x) = 2x "1 ; !f 1
2( ) = 0 36. a. Horizontally, washers. b. Horizontally, prisms. c. Vertically, disks.
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Chapter 8 Solutions Calculus
37. a. A disk (thin cylinder), with thickness !y or dy . b. y c. ! ( y )2dy = ! ydy = ! " y2
2
10
00
10
#010
# = 50! un3
d. The inverse functions is y = x : ! ( x )2dx = ! " x22
10
00
10
# "50! un3 38. a. Since most of the region is closer to the y-axis than the x-axis, one should suspect the
volume of the rotation about the x-axis to have greater volume b. Each figure is the shape of a mostly hollow cone. For rotation about the x-axis, the inner
and outer radii are x2 and 2x and the width is !x :U = (" (2x)20
2
# $ " (x2 )2 )dx
= ! (4x2 " x4 )dx = ! # 43x3 " ! x
5
50
2
$2
0=32!3
" 32!5
=64!15
% 13.404 un3 .
For rotation about the y-axis, the inner and outer radii are y2
and y and the width is
!y = V = ((" ( y )2 # " (y
2)2
0
4
$ )dy = " (y #y2
4)dy = "
y2
2# "
y3
12
4
00
4
$!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!= 8" # 16
3" = 8
3" % 8.378 un3
c. Most of the region is closer to the y-axis and further from the x-axis. So even though the 2nd integral is twice as long (0 to 4), the radii are about 1
2 the size of the radii of
the 1st integral, and within the integral the radii are squared. 39. These are washers with inner and outer radii of 2 ! x and 4 ! x2
and width !x :V = (" (4 # x2 )2 # " (2 # x)2 )dx#1
2
$
= " (16 # 8x2 + x4 # 4 # 4x # x2 )dx#1
2
$
= " (x4 # 9x2 + 4x +12)dx#1
2
$
= " ( x5
5# 9x
3
2+4x2
2+12x)
2
#1
= " (14.4 # (#7.2)) = 21.6" % 67.858 un3
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Chapter 8 Solutions Calculus
40. a. ! (x3 +1)2dx"1
1
# = ! (x6 + 2x3 +1"11
# )dx = ! ( x7
7+ 2 $ x
4
4+ x) 1
"1
= ! ( 17+12+1) " ! (" 1
7+12"1) = ! $ 23
14+ ! $ 9
14=3214
! = 167! % 7.181un3
b. A washer. c. The inner radius is 1 (the distance between y = !1 and the x-axis) and the outer
radius is x3 +1! (!1) = x3 + 2 (the distance between y = !1 and f (x) ).
d. (! (x3 + 2)2 " ! #12 )dx = ! x6"1
1
$"11
$ + 4x3 + 4 "1)dx = ! ( x7
7+ x
4+ 3x)
1
"1
= ! ( 17+1+ 3) " ! (" 1
7+1" 3) = 29
7! + 15
7! = 44
7! % 19.747 un3
e. Basically the integral is the same and gives the same answer: (! (x3 + 2)2 " ! #12 )dx =
"1
1
$ 44!7 % 19.747 un3 41. For a disk, it is as if it were a washer with an inner radius of 0. 42. a. U = 9 ! 2x, dU = !2dx : 1
9!2xdx
2
4
" = ! 121UdU = ! 1
2ln U
4
x=2x=2
4
"
= ! 12ln 9 ! 2x
4
x=2= ! 1
2# (0) + 1
2# ln 5 = 1
2ln 5
b. = 2 ! x66+ 3 ! x
3
3+ x
3
"3=
x6
3+ x
3+ x
3
"3= 243+ 27 + 3" (243" 27 " 3) = 60
c. = (x!1)(x+1)x!1
dx = ! (x +1)dx2
3
"32
" = ! x2
2+ x( ) 32 = ! 92 + 3( ) + (2 + 2) = ! 72
d. = 4x3 2dx1
4
! = 4 " x5 2
5/2
4
1=85" x5 2
4
1=85" (32 #1) = 8"31
5=2485
e. U = sin x, dU = cos xdx : sin3 x cos xdx! 4
! 2
" = U 3dUx=! 4! 2
"
!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!=U4
4
! /2
x=! /4=sin4 x4
! /2
! /4=14#( 2 2)4
4=14# 116
=316
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Chapter 8 Solutions Calculus
43. a. = (3x+1)!6"3!(6x"2)(3x+1)2
=18x+6"18x+6
(3x+1)2=
12
(3x+1)2
b. = sec(5 ln x) tan(5 ln x) ! 5x
c. x32 cos(2x)!3x2 sin(2x)x6
=2x cos(2x)!3 sin(2x)
x4
d. = 2k !93k"1 + k2 ! (ln 9) !93k"1 ! 3 = 2k !93k"1 + (3 ln 9)k293k"1 e. = (2 sin x cos x) cos x + sin2 x(! sin x) = 2 sin x cos2 x ! sin3 x
or 2 sin x(1! sin2 x) ! sin3 x = 2 sin x ! 3sin3 x 44. a. s(0) = 136 ft b. !s (t) = "32t +120 , so initial velocity is !s (0) = 120 ft/s, which is just the t term. c. !s (t) = "32t +120 = 0,120 = 32t, t = 120
32=308=154= 3 3
4sec
d. s(154) = !16(15
4)2 +120(15
4) +136 = !225 + 450 +136 = 361 ft
e. 0 = s(t) = !16t2 +120t +136, 0 = !2t2 +15t +17 = (!2t +17)(t +1),t =
172
: "s (172
) = !32(172
) +120 = !272 +120 = !152 m/s: it will explode.
45. Let x be the total price deduction, so the charge is 159 ! x , the occupancy is 265 + 2x , and
the revenue is (159 ! x)(265 + 2x) .
0 = d
dx((159 ! x)265 + 2x)) = d
dx(159 "265 ! 265x + 318x ! 2x2 )
=d
dx(159 "265 + 53x ! 2x2 ) = 53! 4x, x = 53
4= $13 1
4
So they should charge 159 !13 14= $145.75 .
46. a. k = 1
2 (by symmetry) b. k = 1
c. k = !1 d. k = 1
-
Chapter 8 Solutions Calculus
47. a. y = x ! x3 , "y = 12(x ! x3)!1 2 # (1! 3x2 ) = 1!3x
2
2 x!x3 or 1!3x2
2y
b. When the denominator from part (a) is 0. and y = 0 at each of these points.
c. x = 0,1, !1 48. The vertex is (0, 0): the distance is d(t) = (y ! 0)2 + (x ! 0)2 = (x2 )2 + x2 = x4 + x2 , so
d
dtd(t) = d
dtx4+ x
2 , !d (t) = 12(x4 + x2 )"1 2 # (4x3 + 2x) # x1 (by the extended Chain Rule.
!d ("3) = 12
(81+ 9)"1 2 # ("4 #27 " 6) # (0.5) = 12 90
# ("114) # 12=
"57
2 90=
"57
6 10$ "3.004 units/s
or 3.004 units is also appropriate. 49. a. The shape is a cylinder with a whirlwind cut out of it. A slice is a washer with inner
and outer radii of x2 and 4 and width !x .
V = (! " 42 # ! (x2 )2 )dx
0
2
$ = (16 # x4 )dx = ! (16x # x5
5)2
00
2
$
= ! (32 # 325) = 128!
5% 80.425 un3
b. The shape is like a bowl. A slice is a disk with radius y and width !y . V = ! ( y )2dy = ! ydy
0
4
"04
" = ! #y2
2
4
0= 8! $ 25.133un3
c. The shape is almost like a quarter of a donut and will be hard to draw. A slice is a washer with inner and outer radii of 1+ x2 and 5 and width !x .
V = (! "52 # ! (1+ x2 )2 )dx = ! (25 #1# 2x2 # x4 )dx
0
2
$02
$ = ! (24x # 2 " x3
3# x
5
5)2
0
= ! (48 # 163# 325) = ! (544
15) = 544!
15% 113.935 un3
d. Again this is like a quarter donut. A slice is a washer with inner radius r ! y and outer radius 3 and width ! y .
V = (! " 32 # ! (3# y )2 )dy
0
4
$ = ! (9 # 9 + 6 y # y)dy04
$ = ! (6 y # y)dy04
$
= ! (6 "y3 2
3 2#y2
2)4
0= ! (4 " y3 2 #
y2
2)4
0= ! (32 # 8) # 0 = 24! % 75.398 un3
0 = 2 x ! x3
0 = x ! x3
0 = x(1! x2 )
0 = x(1! x)(1+ x)
x = 0,1, !1
-
Chapter 8 Solutions Calculus
50. a. The radius of the outside cylinder is 5. The radii of the inside disks are y = 2x +1 . ! 52
0
2
" dx # ! (2x +1)202
" dx = ! (25 # 22x # 2 $2x #1)02
" dx = ! (24 # 22x # 2x+1)dx02
"
= ! 24x # 22x
2 ln 2# 2
x+1
ln 2( ) 20 = ! (48 # 162 ln 2 # 8ln 2 ) # (0 # 12 ln 2 # 2ln 2( )= ! 48 # 27
2 ln 2( ) % 28.524 un3
b. The radius is x, but y = 2x +1 or x = ln(y!1)ln 2
.
! x22
5
" dy = !ln(y#1)ln 2( )2
5
"2
dy $ 17 un3
c. ! (52 " (5 " (2x +1))20
2
# )dx = ! (25 " (16 " 8 $2x + 22x )02
# )dx = ! (9 + 8 $2x " 22x02
# )dx
= ! 9x + 8$2x
ln 2" 2
2x
2 ln 2( ) 20 % 41.804! % 131.333un3
d. The radius is x + 1, but y = 2x +1 or x = ln(y!1)ln 2
.
! (x +1)2 "12( )2
5
# dy = ! ln(y"1)ln 2 +1( )2
"12$%&
'()2
5
# dy * 15.75! * 40 un3
e. The radius of the outside cylinder is 7. The radii of the inside disks are y + 2 = 2x + 3 . ! 72
0
2
" dx # ! (2x + 3)202
" dx $ 135.75 un3 51. a. This is a sideways bowl. A slice is a disk with radius x and width ! x . V = ! ( x )2dx = ! xdx = ! " x2
20
4
#04
#4
0= 8! $ 25.133un3 .
b. This is a cylinder with a whirlwind cut out. A slice is a washer with inner and outer radii of y2 and 4 and width dy.
V = (! " r2 # ! (y2 )2 )dy
0
2
$ = ! (16 # y4 )02
$ dy = ! (16y #y5
5)2
0= ! (32 # 32
5) = 128!
5
% 80.425 un3
c. It is like a quarter donut. A slice is a washer with inner and outer radii of 2 + y2 and 6 and width ! y .
V = (! "62 # ! (2 + y2 )2 )dy
0
2
$ = ! (36 # 4 # 4y2 # y4 )dy02
$ = ! (32y # 4 #y3
3#y5
5)2
0
= ! (64 # 323# 325) = 704!
15% 147.445 un3
d. It is like a quarter donut. A slice is a washer with inner and outer radii of 5 ! x and 5 and width ! x .
V = (! "52 # ! (5 # x )2 )dx
0
4
$ = ! (25 # 25 +10 x # x)dx04
$= ! (10 x # x)dx
0
4
$ = ! " (10 " x3/2
3 2# x
2
2)4
0! (20
3"8 # 8) = 136!
3% 142.419 un3
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Chapter 8 Solutions Calculus
52. a. ! (3x +1)2dx0
2
" # 166.421un3
b. The outer radius is 2, the inner radius is x. Since y = 3x +1 , x = ln(y!1)ln 3
. The outside cylinder is solid from y = 0 to y = 2, so we only need to subtract out the inside from y = 2 to y = 10.
! 22dx0
10
" # !ln(y#1)ln 3( )
2
dy2
10
" $ 40! #16.5! = 23.5! $ 73.827 un3
c. The outer radius is (3x +1) +1 = 3x + 2 , the inner radius is 1. ! (3x + 2)2dx
0
2
" # ! (1)2dx02
" $ 73.54! # 2! $ 224.74 un3
d. This would give an unwanted middle term as well as the limits of integration would be incorrect.
53. This is the inside half of a donut (half torus). It will have a cylindrical exterior and a
donuts interior. A slice is a washer with inner and outer radii of 2 ! 1! x2 and 2 and width ! x . V = (! "22 # ! (2 # 1# x2 )2 )
#1
1
$ dx = ! (4 # 4 + 4 1# x2 # (1# x2 ))dx#11
$
= ! (4 1# x2 #1+ x2 )dx#1
1
$ % ! " 4.950 % 15.550!un3
54. a. Vertical slices: disks with radius f (x) and width dx. V = ! ( f (x))2dx
"1
2
# .
b. Vertical slices: washers with inner and outer radii of 1 and 1+ f (x) and width dx. V = (! (1+ f (x))2 " ! (1)2
"1
2
# )dx or ! (2 f (x) + f (x)2 )dx"12
# .
c. Horizontal slices: disks with radius g(y) and width dy. V = ! (g(y))2dy1
3
" .
d. Horizontal slices: washers with inner and outer radii of 5 ! g(y) and 5 and width dy. V = (! "52 # ! (5 # g(y))2 )dy
1
3
$ or ! (10g(y) " g(y)2 )dy13
# . 55. a. A typical slice is a horizontal disk with radius 6
y!
5
y2 and width dy.
V = !1
13
" (6y #5
y2)2dy = ! (36y#2 # 60y#3 + 25y#4 )dy
1
13
"
= ! (36 $y#1
#1# 60 $
y#2
#2+ 25 $
y#3
#3
13
1= ! (#36
y+
30
y2# 25
3y3)
13
1% 36.875 in.3
b. Height is 12: V = ! r2h = ! r2 "12 = 36.875, r2 = 36.87512!
, r = 36.87512!
# 0.989 in.
-
Chapter 8 Solutions Calculus
56. a. y = h ! hrx (slope is 0!h
r!h=
!h
r) or hx + ry = rh or x = r ! r
hy .
b. Using x = r ! rhy as the radius of a disk, V = ! (r " r
hy)2dy
0
h
# .
c. Yes: V = ! (r " rhy)2dy
0
h
# = ! (r2 " 2 r2
hy + r
2
h2y2
0
h
# )dy = ! r2 (1" 2y
h+y2
h2)dy
0
h
#
= ! r2(y "y2
h+
y3
3h2)h
0= ! r2(h " h
2
h+
h3
3h2) = ! r2(h
3) = ! r
2h3
57. Now we have washers with inner and outer radii of 1 and 1+ 6
y!
5
y2
V = (! (1+ 6y" 5y2
)21
13
# " ! $12dy = ! (1+ 36y2113
# + 25y4 +12y" 10y2
" 60y3
"1)dy
= ! (12y"1 + 26y"2 " 60y"3 + 25y"4 )dy1
13
# = ! (12 ln y + 26"1 y"1 " 60 $y"2
"2+ 25 $
y"3
"3)
13
1
= ! (12 ln y " 26y"1 + 30y"2 " 253
)13
1% 104.572 in.3
58. a. The graph of x ! 4 is symmetric about x = 4 , so
x ! 4 dx0
8
" = 2 (x ! 4)dx = 2( x2
2! 4x)
8
44
8
" = 2 # (32 ! 32 ! (8 !16)) = 2 #8 = 16 (This is easily found as the area of two triangles.)
b. = (w3 ! 2)dw = w44
! w2
2+ C"
c. = ! !7dx!5
!1
" = 7dx = 4 # 7 = 28!5!1
" , area of a rectangle.
d. This is a quarter circle: ! "524
=25!
4.
59. Each doll is like a slice of the largest doll, so that when you add up all their volumes,
ideally you will get the full volume of the largest doll. 60. sum = 2! xdx = 2! " x2
2
r
0= ! x2
0
r
#r
0= ! r2 = area of a circle.
61. Rotating y = r2 ! x2 about the x-axis yields disk slices with radius r2 ! x2 and width dx:
V = ! ( r2 " x2 )2dx ="r
r
# (r2 " x2 )dx = ! (r2 $ x " x3
3)
r
"r"r
r
# = ! ((r3 " r3
3) " ("r3 + r
3
3))
= ! (2r3 " 23r3) = ! $ 4
3r3 =
43! r3
-
Chapter 8 Solutions Calculus
62. a. Use washers, but with 2 sections (2 integrals). b. y = 0.5x2, 2y = x V = (! (3)2 " ! (1)2 )dy
0
0.5
# + (! (3)20.54.5
# " ! ( 2y )2 )dy
= 8! y0.5
0+ ! (9 " 2y)
0.5
4.5
# dy
= 4! + (! (9y " y2 )4.5
0.5)
= 4! + ! (812" 814) " ! (9
2" 14)
= 4! + 814! " 17
4! = 4! + 64!
4= 20! un3
63. a. Positive slope, concave up: b b. Negative slope, concave down: d c. Positive slope, concave down: c d. Negative slope, concave up: a, e 64. a. Doll shells b. Circumference strips c. He used the circumference of a strip and dx as the rectangles length and width. 65. Note: These are the actual volumes using the shell method. 2! x " f (x)dx
a
b
#
1A. 2! x(x " 2)2dx0
2
# = 2! (x3 " 4x2 + 4x)dx02
# = 2! 14 x4 "43x3 + 2x2( ) 2
0= 83! !un3
1B. In this case the radius is 2 ! x . 2! (2 " x)(x " 2)2dx
0
2
# = 2! ("x3 + 6x2 "12x + 8)dx02
# =
2! " 14x4 + 2x3 " 6x2 + 8x( ) 2
0= 8! !un3
1C. In this case the radius is x +1 .
2! (x +1)(x " 2)2dx
0
2
# = 2! (x3 " 3x2 + 4)dx02
# = 2! 14 x4 " x3 + 4x( )2
0=
2! (4 " 8 + 8) = 8! !un3
2A. 2! x(4 " x)0
4
# dx = 2! (4x " x2 )04
# dx = 2! 2x2 " 13 x3( )4
0= 64
3! !un3
Solution continues on next page.
-
Chapter 8 Solutions Calculus
65. Solution continued from previous page. 2B. In this case the radius is 4 ! x .
2! (4 " x)(4 " x)dx0
4
# = 2! (16 " 8x + x2 )04
# dx = 2! 16x " 4x2 + 13 x3( )4
0=
2! 64 " 64 + 643( ) =
1283
! !un3
2C. In this case the radius is 2 + x . 2! (2 + x)(4 " x)
0
4
# dx = 2! (8 + 2x " x2 )04
# dx = 2! 8x + x2 " 13 x3( )4
0= 160
3! !un3
3A. 2!0
4
" x2dx = 2! 13 x3( )4
0= 128
3! !un3
3B. In this case the radius is 1+ x . 2! (1+ x)(x)
0
4
" dx = 2! (x + x2 )04
" dx = 2! 12 x2 +13x3( ) 4
0= 176
3! !un3
3C. In this case the radius is 4 ! x . 2!
0
4
" (4 # x)(x)dx = 2! (4x # x2 )04
" dx = 2! 2x2 # 13 x3( )4
0= 64
3! !un3
4A. 2!0
4
" x xdx = 2! x3/204
" dx = 2! 25 x5/2( )4
0= 128
5! !un3
4B. In this case the radius is 4 ! x .
2! (4 " x) x
0
4
# dx = 2! (4x1/2 " x3/2 )dx04
# = 2! 83 x3/2 "25x5/2( ) 4
0=
2! 643" 645( ) =
25615
! !un3
4C. In this case the radius is 5 ! x . 2! (5 " x) x
0
4
# dx = 2! (5x1/2 " x3/2 )dx04
# = 2! 103 x3/2 "25x5/2( ) 4
0=
2! 803" 645( ) =
23615
! !un3
66. a. A thin box with length 2! x , width f (x) , and thickness dx. b. 2! x " f (x)dx
c. 2! x " f (x)dxa
b
#
d. 2! x(0.5x2 )dx1
3
" = ! x3)dx13
" = ! x4
4
3
1= ! 81
4# 14( ) = 20! $ 62.832 cm3
-
Chapter 8 Solutions Calculus
67. a. 2x= 1+
1
y
2
x!1 =
1
y
2!xx
=1
y
x2!x
= y
!y = 1"(2#x)#x(#1)(2#x)2
=2
(2#x)2 At (1, 1) it is 2.
b. x2y ! y3 = 82xy + x2 "y ! 3y2 "y = 0
2xy = 3y2 "y ! x2 "y
2xy = "y (3y2 ! x2 )
2xy
3y2 !x2= "y
At (3, 1) it is 1.
68. a. = 2 ! t3/2
3
2
+ t3
3
4
1= 43!8 + 64
3"
4
3+ 13( ) =
96
3"5
3= 91
3
b. U = x2 +1,!dU = 2xdx : x
x2 +1dx! = 12 "
2xdx
x2 +1! =12
dU
U! =12ln U + C = 1
2ln(x2 +1) + C (using substitution)
c. U = cos u,!dU = ! sin du : tan udu!" /4
" /4
# = !! sin u ducos u!" /4
" /4
# = ! dUU!" /4" /4
#= ! ln U
" /4
!" /4=! ln cos u
" /4
!" /4= ! ln 2
2( ) + ln 22( ) = 0
The best way to realize it is 0 is by symmetry (tangent is odd). d. ln(e2x )! dx = 2x dx! = x2 + C 69. E: 2x2dx
1
2
! = 2 " x#1
#1
2
1=
#2x
2
1= #1+ 2 = 1
70. B: This is ! (2x)2 " ! (2x2 )2( )
0
1
# dx = (4x2 " 4x4 )dx01
# 71. D: At x = 0, lim
x!0f (x) = 1 (by graphing of lHopitals rule), so I is false.
As x!",! f (x)! 0 , so II and III are true. 72. D: I is false because !f (b) does not exist. II and III are true.
-
Chapter 8 Solutions Calculus
73. E: The average is 1e!1
(ln x2 )dx1
e
" # 1.164 Without a calculator if one notes that f is concave down in this interval, with endpoints at
(1, 0) and (e, 2), then it is apparent that its average value must be above the average of 0 and 2, i.e., greater than 1.
74. D: (x2 +1)dx0
c
! = (x2 +1)c2
! dxx3
3+ x
c
0=
x3
3+ x
2
c
c3
3+ c =
83+ 2 "
c3
3" c
c3+ 3c = 8 + 6 " c3 " 3c
2c3 + 6c = 14
c3+ 3c " 7 = 0!!!!!#!!!!!c $ 1.406!by!using!a!calculator
75. a. !(x ! 3)2 + 4( ) dx1
4
" = (!x2 + 6x ! 5)dx14
" = ! x3
3+ 3x2 ! 5x
4
1
= ! 643+ 48 ! 20( ) ! ! 13 + 3! 5( ) = 9 un2
b. 2! x("(x " 3)2 + 4)dx1
4
# = 2! ("x3 + 6x2 " 5x)dx14
# = 2! " x4
4+ 6x
3
3" 5x
2
2( ) 41= 2! ("64 +128 " 40) " " 1
4+ 2 " 5
2( )( ) = ! 48 " " 32( )( ) = 99!2 $ 155.509 un3
76. a. It would have two different parts of f (x) as its bounds (radii). b. Shells would only requite one integral, instead of 2 with washers/discs. c. x ranges from 0 to 3. d. radius = 1 + x, height = f (x) = !x2 + 2x + 3
e. 2! (1+ x)("x2 + 2x + 3)dx0
3
# = 2! ("x3 + x2 + 5x + 3)dx03
#= 2! " x
4
4+ x
3
3+ 5x
2
2+ 3x( ) 30 = 2! " 814 + 273 + 452 + 9( ) = 81!2 $ 127.235 un3
77. 2! (x +1)("x2 + 2x + 3" (x +1))dx
"1
2
# = 2! (x +1)("x2 + x + 2)dx"12
# Note: The height is the difference of the two functions.
-
Chapter 8 Solutions Calculus
78. a. See graph at right. Graph is scaled by 10s. 5x0.5 ! 0.1x1.5 = 0
5x0.5 = 0.1x1.5
5 "x0.5
x0.5
= 0.1 "x1.5
x0.5
5 = 0.1x
x = 50 ft
b. V = ! (5x0.5 " 0.1x1.5 )2dx = ! (25x " x2 + .01x3)dx0
50
#050
# = ! (25 $ x2
2" x
3
3+ .01 $ x
4
4)
50
0
= ! (31250 " 1250003
+15625) = ! $5208 13% 16362.462 ft3
c. The 120 aliens take up 10% !16362.462 ft3 " 1636.246 ft3 and the average weight is 13.635 ft3 !
3.5lbs
ft3" 47.724 lbs.
79. a. Vavg = total displacementtotal time = 1200m96sec = 12.5 m/sec
b. d(t) ! 0.000145x4 " 0.0246x3 +1.315x2 "15.808x + 5.582,#d (t) ! 0.000579x3 " 0.0734x2 + 2.629x "15.808
#d (96) ! 69.952 m/s ! 0.069952 km/s $602s/hr ! 251.829 km/hr
Which might be too fast. c. See graph at right. It is a cubic. Between 50 and 70
seconds the competitor does not go far, but then he speeds up again.
80. a. f (x)dx =
c
a
! " f (x)dx = "( f (x)dx +ab
!ac
! f (x)dx) = "(2.5 " 5) = 2.5bc
!
b. 2 f (x)dx = 2( f (x)dx + f (x)dx)b
c
!ab
!ac
! = 2(2.5 " 5) = "5
c. = ! f (x)dx = !( f (x)dx + f (x)dx + f (x)dxc
d
"bc
"ab
"ad
" ) = !(2.5 ! 5 +1.5) = !(!1) = 1
d. 0 81. B: !f (x) = d
dx(x3 "10x2 + 21x) = 3x2 " 20x + 21 = 0, x =
20 400"4(3)#21
6=20 148
6,
max is at x = 20! 1486
=10! 37
3 and is about 12.597 .
t
v(t)
20
20
40 60 80
40
-
Chapter 8 Solutions Calculus
82. C: x2 = 8 + 2xyx2 !82x
= y
y = x2!4
x
!y = 12" 4 # ("1)x"2 = 1
2+
4
x2
!y = 12+
44=
32
at x = 2
83. A: !!!!!!!!! x 1! x2dx
0
1
" !!#!!U = 1! x2, dU = !2xdx
= ! 12
(!2x) 1! x2dx0
1
" = ! 12 UdUx=01
"
= ! 12U3/2
32
= ! 13U 3/2 = ! 1
3(1! x2 )3 2
1
0= ! 1
3(0) + 1
3$1 = 1
3
84. D: !f (x) = "e"x " 3x2 + 6x "10
!!f (x) = e"x " 6x + 6
, which is zero and changes sign at about 1.06 .
85. B (At horizontal tangents the derivative is 0.) 86. a. Shells: V = 2! x(x +1" (x2 " 6x + 7))dx
1
6
#
or 2! x("x2 + 7x " 6)dx1
6
#
b. Washers: V = (! (3+ x +1)2 " ! (3+ x2 " 6x + 7
1
6
# )2 )dx
or ! ((x + 4)2 " (x2 " 6x +10)2 )dx1
6
#
Graph is scaled by 2s. c. Washers: V = (! ("y2 + 3)2 " ! (y2 +1)2 )dy
"1
1
#
or ! ("8y2 + 8)dy"1
1
#
Solution continued on next page.
-
Chapter 8 Solutions Calculus
86. Solution continued from previous page.
d. Shells: V = 2! (2 " y)("y2 + 3" (y2 +1))dy"1
1
#
or 2! (2 " y)("2y2 + 2)dy"1
1
#
e. Disks: V = ! (cos x + 2)2dx
0
2!
" f. Shells: V = 2! x(cos x + 2)dx
0
2!
" g. Washers: V = (! (6 " x)2 " ! (2x )2 )dx
0
2
#
= ! ((6 " x)2 " 4x )dx0
2
#
h. Shells: V = 2! x("x + 6 " 2x )dx
0
2
#
-
Chapter 8 Solutions Calculus
87. a. g(2) = f (t)dt0
2
! = 2 (triangle), g(4) = 2 ! "#22
2= 2 ! 2" (semicircle)
b. No, it is the opposite.
c. f (x)dx =!2
2
" f (t)dt + f (t)dt02
"!20
" = !g(!2) + g(2)
d. Yes, in fact, its derivative is ddx
f (t)dt = f (x)0
x
! in this interval.
e. This is where its derivative changes from positive to negative: x = 2 . f. g(4) = 2 ! 2" and g1(4) = f (4) = !2 , so the tangent line is
y = !2(x ! 4) + 2 ! 2" = !2x +10 = 2" . g. This is where the derivative of f changes sign: x = 0 and 4. 88. a. = yey !ey
y2, using the Quotient Rule.
b. = 12(sin x)!1 2 " cos x , using the Chain Rule.
c. = dd!(5(cos2 ! + sin2 !)) = d
d!(5) = 0 , by simplifying first.
89. D: This is d
dx( x ) = 1
2x!1 2 .
90. A: There are twenty terms, all multiplied by 1
20, which is the width of a rectangle.
91. C: The intersection is at ex = !x + 3 or ex + x ! 3 = 0, x " 0.792 : A ! ("x + 3" ex )dx
0
.792
# = " x2
2+ 3x " ex
0.792
0! "0.145 " ("1) ! 0.855
92. C: It is flat at x = 0 and 2.
93. E: =x12x!1 2( )e x ! 12 x!1 2e x
x=ex (1!x!1 2 )
2x=ex (x! x )
2x2.
94. C: = f (x)dx
a
b
! + ("3)dx = 2b " a + ("3)(b " a) = 2b " a " 3b + 3a = "b + 2aab
!
-
Chapter 8 Solutions Calculus
95. D: I uses cylindrical shells and II uses disks. 96. a. Slice horizontally b. Slice horizontally, but you would get three different similar shapes. c. Slice vertically. d. No convenient way to slice.
97. b. A(i)!xc=1
n
"
c. With an integral: A(x)dxL
R
! The limit of the sums of volumes as the number of slices !" .
100. It does not matter when some cards in a deck protrude out of it; the deck maintains its
volume, as each card has the same height. 101. a. ! (1
2x cos x + 4)2dx
0
5
" b. 2! x(12 x cos x + 4)dx05
"
c. 2! (6 " x)(12x cos x + 4)dx
0
2
# d. (! (12 x cos x +11)2 " ! # 4905
$ )dx 102. D: = !1
1!(3x)2" 3 = !3
1!9x2 by the Chain Rule
103. B: Vavg = 1! (t + sin t)dt = 1!0
!
" ( t2
2# cos t)
!
0=1!(!2
2# (#1) # (#1)) = !
2+2!
. 104. C: !F (5) = 9 " 5 = 2 , but F(!7) is negative on the graph, and !!F (x) = "1
2 9"x is negative.
-
Chapter 8 Solutions Calculus
105. D: dPdt
= 0.02P + 357
dP
0.02P+357= dt
dP0.02P+357! = dt!10.02
ln(0.02P + 357) = t + C
ln(0.02P + 357) = 0.02t + C
0.02P + 357 = e0.02t+C
0.02P = Ce0.02t
0.02P = "357 + Ce0.02t
P = "17850 + Ce0.02t
!17850 + C = 18000C = 35850
P(6) = !17850 + 35850e0.02"6
# 22571
106. D: xy = x(3x !12) : d
dx(x(3x !12)) = d
dx(3x2 !12x) = 6x !12 = 0, x = 2,
minimum product = 2(6 !12) = !12 . 107. The derivative of g is f: D starts out in a positive direction and is flat at a and b. 109. ln xdx
a
b
! ; No, Cavalieris theorem. 108. 1(a): 2 ( 9 ! x2 )2
0
3
" dx = 36!un3
1(b): 2 12( 9 ! x2 )2
0
3
" dx = 18!un3
1(c): 2 2( 9 ! x2 )20
3
" dx = 72!un3
1(d): 2! 12( ) (
129 " x2 )2
0
3
# dx = 92 ! !un3
1(e): 2 12( 9 ! x2 )2
0
3
" dx = 18!un3
1(f): 2 32( 9 ! x2 )2
0
3
" dx = 18 3 !un3
1(g): 2 12
9 ! x2 + 129 ! x2( ) 12 9 ! x2( )0
3
" dx = 34 (9 ! x2 )dx03
" = 272 !un3
1(h): 2 !4( 9 " x2 )2
0
3
# dx = 9! !un3
1(i): 2! (129 " x2 )2
0
3
# dx = 9! !un3
Solution continues on next page.
-
Chapter 8 Solutions Calculus
108. Solution continued from previous page. Note: For number 2, x2 = 9 ! y2 .
2(a): (2x)(2x)dy0
3
! = 4 (9 " y2 )03
! dy = 72!un3
2(b): (2x)(x)dy0
3
! = 2 (9 " y2 )03
! dy = 36!un3
2(c): (2x)(4x)dy0
3
! = 8 (9 " y2 )03
! dy = 144 !un3
2(d): !2
(x)(x)dy0
3
" = !2 (9 # y2 )03
" dy = 9! !un3
2(e): 12
(2x)(2x)dy0
3
! = 2 (9 " y2 )03
! dy = 36!un3
2(f): 12(2x)(x 3)dy
0
3
! = 3 (9 " y2 )03
! dy = 18 3 !un3
2(g): 12(2x + x)(x)dy
0
3
! = 32 (9 " y2 )03
! dy = 27!un3
2(h): !4
(2x)2dy0
3
" = ! (9 # y2 )03
" dy = 18! !un3
2(i): ! (x)(x)dy0
3
" = ! (9 # y2 )03
" dy = 18! !un3
3(a): 2 (3! y)20
3
" dx = 2 (6 ! 2x)203
" dx = 72!un3
3(b): 2 12(3! y)2
0
3
" dx = (6 ! 2x)203
" dx = 36!un3
3(c): 2 2(3! y)20
3
" dx = 4 (6 ! 2x)203
" dx = 144 !un3
3(d): !2
12(3" y)( )
2
0
3
# dx = !8 (6 " 2x)203
# dx = 92 ! !un3
3(e): 12
(3! y)20
3
" dx = 12 (6 ! 2x)203
" dx = 18!un3
3(f): 12
3
2(3! y)2
0
3
" dx =3
4(6 ! 2x)2
0
3
" dx = 9 3 !un3
3(g): 12(3! y) + 1
2(3! y)( )
0
3
" 12 (3! y)( ) dx =38
(6 ! 2x)20
3
" dx = 272 !un3
3(h): !4
(3" y)20
3
# dx = !4 (6 " 2x)203
# dx = 9! !un3
3(i): ! 12(3" y)( )
2
0
3
# dx = !4 (6 " 2x)203
# dx = 9! !un3 Solution continues on next page.
-
Chapter 8 Solutions Calculus
108. Solution continued from previous page.
4(a): (x ! (!3))2dx!3
3
" = (x + 3)2dx!33
" = 72!un3
4(b): 12
(x + 3)2dx!3
3
" = 36!un3
4(c): 2 (x + 3)2dx!3
3
" = 144 !un3
4(d): !2
12(x + 3)( )
2dx
"3
3
# = !8 (x + 3)2dx"33
# = 9! !un3
4(e): 12
(x + 3)2dx!3
3
" = 36!un3
4(f): 12
3
2(x + 3)2dx
!3
3
" =3
4(x + 3)2dx
!3
3
" = 18 3 !un3
4(g): 12(x + 3) + 1
2(x + 3)( )
!3
3
" 12 (x + 3)( ) dx =38
(x + 3)2!3
3
" dx = 27!un3
4(h): !4
(x + 3)2"3
3
# dx = 18! !un3
4(i): ! 12(x + 3)( )
2dx
"3
3
# = !4 (x + 3)2dx"33
# = 18! !un3
5(a): ( x +1)2dx!1
3
" = (x +1)dx!13
" = 8!un3
5(b): 12( x +1)( x +1)dx
!1
3
" = 12 (x +1)dx!13
" = 4 !un3
5(c): 2( x +1)( x +1)dx!1
3
" = 2 (x +1)dx!13
" = 16!un3
5(d): !2
12
x +1( )2dx
"1
3
# = !8 (x +1)dx"13
# = ! !un3
5(e): 12( x +1)( x +1)dx
!1
3
" = 12 (x +1)dx!13
" = 4 !un3
5(f): 12( x +1)(
3
2x +1)dx
!1
3
" =3
4(x +1)dx
!1
3
" = 2 3 !un3
5(g): 12!1
3
" x +1 + 12 x +1( ) 12 x +1( ) dx = 38 (x +1)!13
" dx = 8!un3
5(h): !4( x +1)2dx
"1
3
# = !4 (x +1)dx"13
# = 2! !un3
5(i): ! 12
x +1( )2dx
"1
3
# = !4 (x +1)dx"13
# = 2! !un3
Solution continues on next page.
-
Chapter 8 Solutions Calculus
108. Solution continued from previous page.
6(a): 2 (3sin x)2dx0
3
! = 18 (sin x)203
! dx " 28.26!un3
6(b): 2 (3sin x) 32sin x( ) dx
0
3
! = 9 (sin x)203
! dx " 14.13!un3
6(c): 2 (3sin x)(6 sin x)dx0
3
! = 36 (sin x)203
! dx " 56.52!un3
6(d): 2 !2(3 sin x)2dx
0
3
" = 9! (sin x)203
" dx # 14.13! !un3
6(e): 2 12(3 sin x)(3 sin x)dx
0
3
! = 9 (sin x)203
! dx " 14.13!un3
6(f): 2 12(3 sin x)(
3 3
2sin x)dx
0
3
! =9 3
2(sin x)2
0
3
! dx " 12.24 !un3
6(g): 2 12(3 sin x + 3
2sin x)( 3
2sin x)dx
0
3
! = 274 (sin x)203
! dx " 10.60!un3
6(h): 2 !4(3 sin x)2dx
0
3
" = 92 ! (sin x)203
" dx # 7.065! !un3
6(i): 2 ! (3 sin x)2dx0
3
" = 18! (sin x)203
" dx # 28.26! !un3
Note: For number 7 the radius/length is (3! x) , where x = y2 !1 . Thus r = (4 ! y2 ) .
7(a): (3! x)20
2
" dy = (4 ! y2 )2dy02
" = 17 115 =25615
!un3
7(b): (4 ! y2 ) 12(4 ! y2 )( ) dy
0
2
" = 12 (4 ! y2 )2dy02
" = 25630 !un3
7(c): (4 ! y2 ) 2(4 ! y2 )( ) dy0
2
" = 2 (4 ! y2 )2dy02
" = 51215 !un3
7(d): !2
12(4 " y2 )( )
2dy
0
2
# = !8 (4 " y2 )2dy02
# = 3215 ! !un3
7(e): 12(4 ! y2 )(4 ! y2 )dy
0
2
" = 12 (4 ! y2 )2dy02
" = 25630 !un3
7(f): 12(4 ! y2 ) 3
2(4 ! y2 )( ) dy
0
2
" =3
4(4 ! y2 )2dy
0
2
" =64 3
15!un3
7(g): 12(4 ! y2 ) + 1
2(4 ! y2 )( ) 12 (4 ! y2 )( ) dy0
2
" = 38 (4 ! y2 )2dy02
" = 325 !un3
7(h): !4(4 " y2 )2dy
0
2
# = !4 (4 " y2 )2dy02
# = 6415 ! !un3
7(i): ! 12(4 " y2 )( )
2dy
0
2
# = !4 (4 " y2 )2dy02
# = 6415 ! !un3 Solution continues on next page.
-
Chapter 8 Solutions Calculus
108. Solution continued from previous page.
8(a): (3! x)2dy!3
3
" = (3! y)2dy!33
" = 72!un3
8(b): 12
(3! y)(3! y)dy!3
3
" = 36!un3
8(c): 2 (3! y)2dy!3
3
" = 144 !un3
8(d): !2
12(3" y)( )
2dy
"3
3
# = !8 (3" y)2dy"33
# = 9! !un3
8(e): 12
(3! y)2dy!3
3
" = 36!un3
8(f): 12
3
2(3! y)2dy
!3
3
" =3
4(3! y)2dy
!3
3
" = 18 3 !un3
8(g): 12(3! y) + 1
2(3! y)( )
!3
3
" 12 (3! y)( ) dy =38
(3! y)2!3
3
" dy = 27!un3
8(h): !4
(3" y)2"3
3
# dy = 18! !un3
8(i): ! 12(3" y)( )
2dy
"3
3
# = !4 (3" y)2dy"33
# = 18! !un3
Note: For number 9 the radius/length is 2x = y + 3.
9(a): (y + 3)2!3
3
" dy = 72!un3
9(b): 12(y + 3)(y + 3)
!3
3
" dy = 36!un3
9(c): 2(y + 3)(y + 3)!3
3
" dy = 144 !un3
9(d): !2x2
"3
3
# dy = !212(y + 3)( )
"3
3
#2
dy = !8
(y + 3)2"3
3
# dy = 9! !un3
9(e): 12(y + 3)(y + 3)
!3
3
" dy = 36!un3
9(f): 12(y + 3) 3
2(y + 3)( )!3
3
" dy =3
4(y + 3)2
!3
3
" = 18 3 !un3
9(g): 12(y + 3) + 1
2(y + 3)( )
!3
3
" 12 (y + 3)( ) dy =38
(y + 3)2!3
3
" dy = 27!un3
9(h): !4(y + 3)2dy
"3
3
# = 18! !un3
9(i): ! x2"3
3
# dy = ! 12 (y + 3)( )"33
#2
dy = !4
(y + 3)2"3
3
# dy = 18! !un3
-
Chapter 8 Solutions Calculus
110. The radius is x. x = y ( y )20
9
! dy 111. ( x )2
0
4
! dx = x04
! dx = 12 x24
0=162
" 0 = 8 un2 112. 2 (2(4 ! x2 ))2
0
2
" dx 113. dl = 6,!dw = 2,!A = lw,!dA = (dl)w + l(dw) = 6(15) + 30(2) = 90 + 60 = 150 cm2 /sec 114. a. Use integration by parts. Let u = x!!!!!1dx and dv = (2x !1)!1/2dx!!"!!(2x !1)1/2 .
x(2x !1)1/2 ! (2x !1)1/2dx1
5
"
x(2x !1)1/2 ! 13(2x !1)3/2( ) 5
1= (15 ! 9) ! 1! 1
3( ) = 513= 16
3
b. Let u = 1! x2 !!" du = !2xdx . If x = 1, u = 0. If x = 0, u = 1. u ! 1
2du( )
1
0
" = ! u ! 12 du( )01
" = 122
3u3/2( ) 1
0= 13
c. Let u = x2 +1!!!!!du = 2xdx . If x = 2, u = 5. If x = 0, u = 1. 12u
!du1
5
! = 12 ln u5
1=12(ln 5 " ln1) = 1
2ln 5
d. Let u = !x2 !!"!!du = !2xdx . If x = 2, u = 4. If x = 0, u = 0. ! 32eu
0
!4
" du = 32 eu!40
" du = 32 eu0
!4=3
2! 32e!4
115. a. x
15=42
60!!!!!x = 10.5 cm3
b. V = 13! r3 !!"!!dV = ! r2dr 15 = ! (1.7)2dr !!"!!dr = 15
! (1.7)2= 1.652 cm/sec
c. Only if it is chocolate. 116. !g (x) = 1
!f (g(x))!!"!! !g (3) = 1
!f (g(3))=
1!f (1)
=12
-
Chapter 8 Solutions Calculus
117. The average rate is the average slope. y(8) = 12(8)2 + 2(8) +1 = 49 ,
y(0) = 12(0)2 + 2(0) +1 = 1. m = 49!1
8!0= 6
The slope is !y (t) = t + 2 . t + 2 = 6!!!!!t = 4 118. a. This is !y at x = 6 if y = ln(x ! 4) . !y = 1
x"4=
1
6"4=1
2
b. This is !y at x = 25 if y = 2x !1 . !y = 12 2x"1
=1
2 49=1
14
c.
limx!"
sin2 xx
= limx!"
sin xx
!i! limx!"
(sin x) = 0 because limx!"
sin x
x= 0
d. 3x > ex since 3 > e . Therefore limx!"
3x +7x
ex+10x
!" . 119. a. y = 4 ! x
3 (the slope is ! 4
12= !
1
3)
b. y22
!dx = (4 " x3)2dx
c. 12
(4 ! x3)2dx = 1
!2(!3)
(4!x 3)3
30
12
"12
0= ! 1
2(4 ! x
3)3
12
0= !0 + 1
243 = 32 cm3
120. a. !
2
x
2( )04
"2
dx b. 9 ! x2( ) 9!x22"#$
%&'0
3
( !dx
c. y2( )2
dy !y
2! 4y !16( )
4
8
"04
"2
dy 121. a. For a given y, y = 0.05(x + 50)2, 20y = (x + 50)2, 20y = x + 50, x = 20y ! 50 , so
the length is 2 ! (50 " 20y ) = 100 " 4 5y , so a slice has volume (100 ! 4 5y )2dy . b. (100 ! 4 5y )2dy = (10000 ! 800 5y + 80y)dy
0
12
"012
"
= 1000y ! 80 5y3 2
3 2+ 40y2
12
0# 76186 yards3
c. Full volume is (100 ! 4 5y )2dy = 10000y ! 1600 53
y3 2 + 40y220
00
20
"
= 109333 13
yards3, so there are about 109333 13! 76186 " 33147.5 yards3 left,
33147.5 yrds3
60 yrds3 /day= 552.5 days left, 1.514 years left, so no delay.
-
Chapter 8 Solutions Calculus
122. b. y = h ! hb 2
x = h ! 2hbx or 2h
bx = h ! y, x = b
2!
b2hy
c. [2(b2! b2hy)]2
0
h
" dy = (b ! bh y)2dy0h
" = ! hb #13(b ! b
hy)3
h
0= !0 + h
b# 13#b3 = 1
3b2h
123. b. The length and width of the squares is x. x = !2y + 20
(20 ! 2y)2dy = (400 ! 80y + 4y2 )dy0
10
" = 400y ! 40y2 + 43 y310
0=40003un3
0
10
" 124. !y = "1
(1+x2 )2#2x = "2x
(1+x2 )2 by the Chain Rule.
At x = !1 we have y = 12
and !y = 12
so the tangent line is y = 12(x +1) + 1
2=12x +1 .
At x = 2 , we have y = 15
and !y = "425
, so the tangent line is y = ! 425(x ! 2) + 1
3.
Therefore 12x +1 = ! 4
25(x ! 2) + 1
5, 25x + 50 = !8x +16 +10, 33x = !24, x = !24
33,
y = 12(!2433) +1 = 21
33: (!2433, 2133) " (!0.727, 0.636)
125. a. x ! 4dx = (x!4)3 2
3 2
8
44
8
" = 43 2
3 2=163un2
b. x ! 4dx = x ! 4
c
8
"4c
" dx,(x!4)3 2
3 2
c
4=(x!4)3 2
3 2
8
c,(c!4)3 2
3 2! 0 = 16
3!(c!4)3 2
3 2,
43(c ! 4)3 2 = 16
3, (c ! 4)3 2 = 4, c ! 4 = 43 2, c = 4 + 42 3 # 6.520
c. ! ( x " 4 )2dx4
8
# = ! (x " 4)dx = ! ( x2
2" 4x)
8
44
8
# = ! (32 $ 32 " (8 "16)) = 8! un3 using disks.
d. ! ( x " 4 )2dx = !d
8
#4d
# ( x " 4 )2dx
! ( x2
2" 4x)
d
4= ! ( x
2
2" 4x)
8
d
! (d2
2" 4d " ("8)) = ! (0 " (d
2
2" 4d))
d2
2" 4d + 8 = " d
2
2+ 4d
d2 " 8d + 8 = 0
d =8+ 64"4(8
2= 4 +
32
2= 4 +
4 2
2= 4 + 2 2 $ 6.828
126. A: V = ( 4 ! x )2dx
0
4
" = (4 ! x)dx04
" = (4x ! x2
2)4
0= 16 ! 8 = 8
-
Chapter 8 Solutions Calculus
127. C: ddx(x2 + y2 ) = d
dx(25)
2x + 2y !y = 0
2y !y = "2x
y ' = "xy
ddx( !y ) = d
dx(" x
y)
!!y =y("1)" !y ("x)
y2=
"y+x !y
y2=
"y+x(" x y)
y2
="y2 "x2
y3=
"(x2 +y2 )
y3=
"25
y3
128. For x in (2, 2), !f (x) = 1
4"x2# ("2x) = "2x
4"x2.
For x > 2 or x < !2 , ddxf (x) = d
dxln(x2 ! 4) = 1
x2 !4"2x = !2x
4!x2.
We get the same answer: D. 129. E: !f (x) = " 1
x2" 8x + 7, !!f (x) = "("2) # 1
x3" 8 = 2
x3" 8 , which is zero when
2
x3= 8, 2
8= x
3=14, x = (2!2 )1 3 = 2!2 3 , and undefined at x = 0 it is positive for x in the
interval (0, 2!2 3) . 130. C: 4ydy = (2x ! 3)dx
4ydy = (2x ! 3)dx""2y2 = x2 ! 3x + C
y2 = x2
2! 3xx + C
y = x2
2! 32x + C
2 = 12!32+ C
4 = !1+ C
C = 5
y = x2
2!32x + 5, f (2) = 2 ! 3+ 5 = 2
131. E: !y = 4x3 + 9x2, !y (0) = 0 , so the normal line is vertical; x = 0 . 132. The real length is 1+ (2x)2dx ! 33.637
"4
4
# , so hopefully students will get answers between 30 and 35, for example, by using secants.
133. The more secants that are used, the better they approximate the curve, so that the estimated
arc length becomes more accurate.
134. a. (! x)2 + (! yi )2 b. (! x)2 + (! yi )2i=1
n
!
-
Chapter 8 Solutions Calculus
135. a. As ! x! 0 , the secant line approaches a line tangent to f (x) and xi , so the slope of the secant line approaches the slope of f (x) .
b. dydx
at xi; !f (xi )
c. ! yi! x
! "f (xi ), ! yi ! ! x # "f (xi ) ! ! x #2xi (since ddx (x2 ) = 2x )
d. arc length ! ! x2 + (2 ! x " xi )2i=1
50
# = ( 850 )2+ [2 " 8
50" ($4 + 8i
50)]2
i=0
49
#
= ( 425
)2 + ( 825
)2($4 + 4i25
)2
i=0
49
# ! 33.646 units
136. a. limn!"
! x2+ (2! x # xi )
2
i=1
n
$ = limn!"
(8n)2 + (16
n# (%4 + 8i
n))2
i=0
n%1
$
b. limn!"
(1+ 4xi2)! x2
i=1
n
# = limn!"
1+ 4xi2
i=1
n
# ! x = 1+ 4x2$4
4
% dx
c. ! 33.637 , so the approximation was off by a little less than 0.01(! 0.009) .
137. a. limn!"
! x2 + ! yi2
i=1
n
# = limn!"
1+ (! yi! x)2
i=1
n
# ! x2 = limn!"
1+ (! yi! x)2
i=1
n
# ! x
b. 1+ ( !f (x))2a
b
" dx 138. a. 1+ cos2 x
0
!
" dx # 3.820 units (by calculator)
b. 1+ (x !1)1/2( )21
9
" dx = 1+ (x !1)19
" dx = x19
" dx = 23 x3/29
1= 54
3! 23= 52
3!units
139. a. !f (x) = ex : 1+ e2x
"2
2
# dx $ 9.010!units (by calculator).
b. !f (x) = 1x
x2 +1
x21
e
" # 2.0035!units (by calculator)
-
Chapter 8 Solutions Calculus
140. ln y = ln ex2 = x2 !!!!!x = ln y,
V = (2 ln y1
e
" )2dy = 4(ln y)dy = 4(y ln y # y)1e
"e
1
= 4(e # e) # 4(0 #1) = 4 !un3
141. xn+1 = xn ! f (xn )"f (xn ) (xn )
"f (x) = ! 1(1+x2 )
#2x = !2x(1+x2 )2
x2 = 1!1 2
1 2= 2
x3 = 3.25, x4 = 5.023,!...
The values keep getting larger, but the function has no root for Newtons Method to approach; only an asymptote of y = 0 .
142. a. Use washers: (! (2x +1)2 " ! (x2 +1)2 )dx
0
2
#
b. Use shells: 2! x(2x +1" (x2 +10
2
# ))dx
c. Use washers: (! (4 " x2 )2 " ! (4 " 2x)2 )dx0
2
#
d. Use shells: 2! (4 " x)(2x +1" (x2 +1))dx0
2
# 143. a. f = x, dg = 5x dx, df = dx, g = 1
ln 5!5x :
x5x dx = xln 55x " 5
x
ln 5dx = x
ln 5!5x " 5
x
(ln 5)2## + C =5x
ln 5(x " 1
ln 5) + C
b. u = ln x +1, du = dxx: ln x+1
xdx
1
e
! = udu =x=1e
! u2
2
e
x=1=(ln x+1)2
2
e
1= 2 " 1
2=32
c. u = x2 ! 4, du = 2xdx : duu=" 12 ln u + C =
12ln x2 ! 4 + C
d. u = x2 + 4, du = 2xdx : xx2 +4
dx =! 12 ln u + C =12ln(x2 + 4) + C
-
Chapter 8 Solutions Calculus
144. a. Vavg = 120 ( (10000 +100t)dt + 10t dt)1020
!010
! = 120 (10000t + 50t210
0) + ( 1
20 ln 1010t
20
10)
= 100250 + 120 ln 10
(1020 "1010 ) # 2.1710 $1018km/hr
b. The Mean Value Theorem does not apply because v is not continuous, but v does equal Vavg at 10t = 2.171 !1018, t = log(2.171 !1018 ) " 18.337sec .
c. aavg = Vfinal!V020seconds = 1020
!1000020
" 5 #1018km/hr/sec d. The Mean Value Theorem does not apply, but a = aavg at
(ln10) !10t = 5 "1018, t = log( 1ln 10
!5 !1018 ) # 18.337sec .