chapter 7 soulutions
TRANSCRIPT
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56. Method 1Compare graph ofy1
x2 lnx with
y2
NDERx3
3
ln x
x
9
3
. The graphs should be the same.Method 2Compare graph ofy
1 NINT(x2 lnx) with
y2
x3
3
ln x
x
9
3
. The graphs should be the same or differ
only by a vertical translation.
57. (a) 20,000 10,000(1.063)t
2 1.063t
ln 2 tln 1.063
tln
l
1
n
.0
2
63 11.345
It will take about 11.3 years.
(b) 20,000 10,000e0.063t
2 e0.063t
ln 2 0.063t
t0
l
.
n
06
2
3 11.002
It will take about 11.0 years.
58. (a) f(x) d
d
x x
0
u(t) dt u(x)
g(x) d
d
x x
3
u(t) dt u(x)
(b) C f(x) g(x)
x0
u(t) dt x3
u(t) dt
x
0
u(t) dt 3
x
u(t) dt
30
u(t) dt
59. (a) y 1 5
5
.8
6
9
.0
4
7
e
1
60.0205x
[20, 200] by [10, 60]
(b) The carrying capacity is about 56.0716 million people.(c) Use NDER twice to solvey 0. The solution is
x 86.52, representing (approximately) the year 1887.The population at this time was approximately
P(86.52) 28.0 million people.
60. (a) T 79.961(0.9273)t
[1, 33] by [5, 90]
(b) Solving T(t) 40 graphically, we obtain t 9.2 sec.The temperature will reach 40 after about 9.2 seconds.
(c) When the probe was removed, the temperature was
about T(0) 79.96C.
61. v
0
k
m coasting distance
(0.86)(
k
30.84) 0.97
k 27.343
s(t) v
0
k
m(1 e(k/m)t)
s(t) 0.97(1 e(27.343/30.84)t)
s(t) 0.97(1 e0.8866t)
A graph of the model is shown superimposed on a graph of
the data.
[0, 3] by [0,1]
Chapter 7
Applications of Definite Integrals
s Section 7.1 Integral as Net Change(pp. 363374)
Exploration 1 Revisiting Example 2
1. s(t) t2 (t8
1)2 dt t3
3
t
8
1 C
s(0) 0
3
3
0
8
1 C 9 C 1
Thus, s(t) t
3
3
t
8
1 1.
2. s(1) 1
3
3
1
8
1 1
1
3
6. This is the same as the
answer we found in Example 2a.
3. s(5) 5
3
3
5
8
1 1 44. This is the same answer we
found in Example 2b.
288 Section 7.1
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Quick Review 7.1
1. On the interval, sin 2x 0 whenx
2, 0, or
2. Test one
point on each subinterval: forx 3
4
, sin 2x 1;
forx
4, sin 2x 1; forx
4, sin 2x 1; and for
x 3
4
, sin 2x 1. The function changes sign at
2, 0,
and
2. The graph is
2. x2 3x 2 (x 1)(x 2) 0 whenx 1 or 2. Test
one point on each subinterval: for x 0, x2 3x 2 2;
for x 3
2, x2 3x 2
1
4; and forx 3,
x2 3x 2 2. The function changes sign at 1 and 2.
The graph is
3. x2 2x 3 0 has no real solutions, since
b2 4ac (2)2 4(1)(3) 8 0. The function is
always positive. The graph is
4. 2x3 3x2 1 (x 1)2(2x 1) 0 whenx 1
2 or 1.
Test one point on each subinterval: for x 1,
2x3 3x2 1 4; forx 0, 2x3 3x2 1 1; and
x 3
2, 2x3 3x2 1 1. The function changes sign at
1
2. The graph is
5. On the interval, x cos 2x 0 whenx 0,
4,
3
4
, or
5
4
.
Test one point on each subinterval: for x
8,
x cos 2x
1
6
2; forx
2, x cos 2x
2; forx ,
x cos 2x ; and forx 4, x cos 2x 0.58. The
function changes sign at
4,
3
4
, and
5
4
. The graph is
6. xex 0 whenx 0. On the rest of the interval, xex is
always positive.
7. x2
x
1 0 whenx 0. Test one point on each subinterval:
forx 1,x2
x
1
1
2; forx 1,
x2
x
1
1
2. The
function changes sign at 0. The graph is
8. x
x
2
2
2
4 0 whenx 2 and is undefined when
x 2. Test one point on each subinterval: forx 5
2,
x
x
2
2
2
4
1
9
7; forx 1.9,
x
x
2
2
2
4 4.13; forx 0,
x
x2
2
4
2
1
2; forx 1.9,
x
x
2
2
4
2 4.13; and forx 5
2,
x
x
2
2
2
4
1
9
7. The function changes sign at 2, 2, 2
and 2. The graph is
9. sec (1 1 sin2x) cos (1
1
cos x) is undefined when
x 0.9633 kor 2.1783 k for any integer k. Test for
x 0: sec (1 1 sin20) 2.4030.
Test forx 1: sec (1 1 sin21) 32.7984. The
sign alternates over successive subintervals. The function
changes sign at 0.9633 kor 2.1783 k, where kis an
integer. The graph is
10. On the interval, sin 1x 0 whenx 31
or
2
1
. Test one
point on each subinterval: forx 0.1, sin 1x 0.54; forx 0.15, sin 1x 0.37; and forx 0.2,sin 1x 0.96. The graph changes sign at 3
1
, and
2
1
.
The graph is
+
0.1 0.213
12
f(x)
x
+ +
2.1783 0.9633 0.9633 2.1783
f(x)
x
+ ++
3 2 2 32 2
f(x)
x
+
5 0 30
f(x)
x
++
0 44
34
54
f(x)
x
+ +
2 2112
f(x)
x
+
4 2
f(x)
x
+ +
2 1 2 4
f(x)
x
++
3 20 2
2
f(x)
x
Section 7.1 289
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Section 7.1 Exercises
1. (a) Right when v(t) 0, which is when cos t 0, i.e.,
when 0 t
2 or
3
2
t 2. Left when cos t 0,
i.e., when
2 t
3
2
. Stopped when cos t 0,
i.e., when t
2 or
3
2
.
(b) Displacement
20
5 cos t dt 5sin t 5[sin 2 sin 0] 0
(c) Distance 20
5 cos t dt
/20
5 cos t dt 3/2/2
5 cos t dt 23/2
5 cos t dt
5 10 5 20
2. (a) Right when v(t) 0, which is when sin 3t 0,
i.e., when 0 t
3
. Left when sin 3t 0, i.e., when
3 t
2. Stopped when sin 3t 0, i.e., when t 0
or
3.
(b) Displacement /20
6 sin 3t dt 613 cos 3t 2cos 32
cos 0 2
(c) Distance /20
6 sin 3t dt
/30
6 sin 3t dt /2/3
6 sin 3t dt 4 2 6
3. (a) Right when v(t)
49
9.8t
0, i.e., when 0
t
5.
Left when 49 9.8t 0, i.e., when 5 t 10.
Stopped when 49 9.8t 0, i.e., when t 5.
(b) Displacement 100
(49 9.8t) dt
49t 4.9t2 49[(10 10) 0] 0
(c) Distance 100
49 9.8t dt
50
(49 9.8t) dt 105
(49 9.8t) dt
122.5 122.5 245
4. (a) Right when
v(t) 6t2 18t 12 6(t 1)(t 2) 0,
i.e., when 0 t 1. Left when 6(t 1)(t 2) 0,
i.e., when 1 t 2. Stopped when
6(t 1)(t 2) 0, i.e., when x 1, or 2.
(b) Displacement 2
0
(6t2 18t 12) dt
2t3 9t2 12t [(16 36 24) 0] 4
(c) Distance 20
6t2 18t 12 dt
10
(6t2 18t 12) dt 21
(6t2 18t 12) dt
5 1 6
5. (a) Right when v(t) 0, which is when sin t 0 and
cos t 0, i.e., when 0 t
2 or
3
2
t 2. Left
when sin t 0 and cos t 0, i.e., when 2 t or
t 3
2
. Stopped when sin t 0 or cos t 0,
i.e., when t 0,
2, ,
3
2
, or 2.
(b) Displacement 20
5 sin2 tcos t dt 513 sin3 t
5[0 0] 0
(c) Distance 20
5 sin2 tcos t dt
/20
5 sin2 tcos t dt 3/2/2
5 sin2 tcos t dt
2
3/2
5 sin2 tcos t dt
5
3
1
3
0
5
3
2
3
0
6. (a) Right when v(t) 0, which is when 4 t 0, i.e.,
when 0 t 4. Left: never, since 4 t cannot be
negative. Stopped when 4 t 0, i.e., when t 4.
(b) Displacement 40
4 t dt 23(4 t)3/2
2
3[0 8]
1
3
6
(c) Distance 40
4 t dt 1
3
6
4
0
2
0
2
0
10
0
/2
0
2
0
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7. (a) Right when v(t) 0, which is when cos t 0,
i.e., when 0 t
2 or
3
2
t 2. Left when
cos t 0, i.e., when
2 t
3
2
. Stopped when
cos t 0, i.e., when t
2 or
3
2
.
(b) Displacement 20
esin tcos t dt esin t [e0 e0] 0
(c) Distance 20
esin tcos t dt /20
esin tcos t dt
3/2/2
esin tcos t dt 23/2
esin tcos t dt
(e 1) e 1e 1 1
e 2e 2e 4.7
8. (a) Right when v(t) 0, which is when 0 t 3. Left:
never, since v(t) is never negative. Stopped when t 0.
(b) Displacement 30
1
t
t2 dt 12 ln (1 t2)
1
2[ln (10) ln (1)]
ln
2
10
1.15
(c) Distance 30
1
t
t2 dt
ln
2
10 1.15
9. (a) v(t) a(t) dt t 2t3/2 C, and since v(0) 0,v(t) t 2t3/2. Then v(9) 9 2(27) 63 mph.
(b) First convert units:
t 2t3/2 mph 36
t
00
1
t
8
3
0
/2
0 mi/sec. Then
Distance 90
36
t
00
1
t
8
3
0
/2
0
dt
72t
0
2
0
4
t
5
5
0
/2
0 8
9
00
5
2
0
7
0 0 0.06525 mi
344.52 ft.
10. (a) Displacement 40
(t 2) sin t dt
sin t tcos t 2 cos t [(sin 4 4 cos 4 2 cos 4) 2] 1.44952 m
(b) Because the velocity is negative for 0 t 2, positive
for 2 t , and negative for t 4,
Distance 20
(t 2) sin t dt 2
(t 2) sin t dt
4
(t 2) sin t dt
[(2 sin 2) ( sin 2 2)
( 2 cos 4 sin 4 2)]
2 2 cos 4 2 sin 2 sin 4 2 1.91411 m.
11. (a) v(t) a(t) dt 32 dt 32t C1, where
C1
v(0) 90.
Then v(3) 32(3) 90 6 ft/sec.
(b) s(t) v(t) dt 16t2 90t C2, where
C2
s(0)
0. Solve s(t)
0:
16t2 90t 2t(8t 45) 0
when t 0 or t 4
8
5 5.625 sec.
The projectile hits the ground at 5.625 sec.
(c) Since starting height ending height,
Displacement 0.
(d) Max. Height s5.6225
16
5.6
2
25
2
90
5.6
2
25
126.5625, andDistance 2(Max. Height) 253.125 ft.
12. Displacement c0
v(t) dt 4 5 24 23 cm
13. Total distance c0
v(t) dt 4 5 24 33 cm
14. At t a, s s(0) a0
v(t) dt 15 4 11.
At t b, s s(0) b0
v(t) dt 15 4 5 16.
At t c, s s(0)
c
0
v(t) dt 15 4 5 24 8.
15. At t a, where d
d
v
t is at a maximum (the graph is steepest
upward).
16. At t c, where d
d
v
t is at a maximum (the graph is steepest
upward).
17. Distance Area under curve 412 1 2 4(a) Final position Initial position Distance
2 4 6; ends atx 6.
(b) 4 meters
18. (a) Positive and negative velocities cancel: the sum of
signed areas is zero. Starts and ends atx 2.
(b) Distance Sum of positive areas 4(1 1) 4meters
4
0
9
0
3
0
2
0
Section 7.1 291
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19. (a) Final position 2 70
v(t) dt
2 1
2(1)(2)
1
2(1)(2) 1(2)
1
2(2)(2)
1
2(2)(1)
5;
ends atx 5.
(b) 70
v(t) dt 12(1)(2)
1
2(1)(2) 1(2)
1
2(2)(2)
1
2(2)(1)
7 meters
20. (a) Final position 2 100
v(t) dt
2 1
2(2)(3)
1
2(1)(3) (3)(3)
1
2(1)(3)
1
2(3)(3)
2.5;
ends atx 2.5.
(b) Distance 100
v(t) dt
1
2(2 3)
1
2(1)(3) 3(3)
1
2(1)(3)
1
2(3)(3)
19.5 meters
21. 100
27.08 et/25 dt 27.0825et/25 27.08[25e0.4 25]
332.965 billion barrels
22. 2403.9 2.4 sin 1
2
t dt 3.9t28
.8 cos 1
2
t
93.6 28.8 28.8 93.6 kilowatt-hours23. (a) Solve 10,000(2 r) 0: r 2 miles.
(b) Width r, Length 2r: Area 2rr
(c) Population Population density Area
(d) 20
10,000(2 r)(2r) dr 20,0002
0
(2r r2) dr
20,000r2 13r3 20,0004 8
3 0
80,
3
000 83,776
24. (a) Width
r, Length
2
r: Area
2
r
r
(b) Volume per second
Inches per second Cross section area
8(10 r2)s
i
e
n
c
. (2r)rin
2 flow in
s
in
ec
3
(c) 30
8(10 r2)(2r) dr 163
0
(10r r3) dr
165r2 14r4 1645 84
1 0
396s
in
ec
3
1244.07 s
in
ec
3
25. (Answers may vary.)
Plot the speeds vs. time. Connect the points and find the
area under the line graph. The definite integral also gives
the area under the curve.
26. (a) Sum of numbers in Sales column 797.5 thousand
(b) Enter the table in a graphing calculator and use
QuadReg: B(x) 1.6x2 2.3x 5.0.
(c) 11
0 (1.6x2
2.3x 5.0) dx
13.6x3
2
2
.3x2 5.0x
904.02 thousand
(d) The answer in (a) corresponds to the area of left hand
rectangles. These rectangles lie under the curveB(x).
The answer in (c) corresponds to the area under the
curve. This area is greater than the area of rectangles.
27. (a) 10.50.5
(1.6x2 2.3x 5.0) dx
13.6x3
2
2
.3x2 5.0x 798.97 thousand
(b) The answer in (a) corresponds to the area of midpointrectangles. The curve now gives a better approximation
since part of each rectangle is above the curve and part
is below.
28. Treat 6 P.M. as 18 oclock:
b
2
n
a f(x0)
n1
i1
2f(xi) f(x
n)
1
2
8
(1
0)
8[120 2(110) 2(115) 2(115) 2(119)
2(120) 2(120) 2(115) 2(112) 2(110)
121]
1156.5
29. F(x) kx; 6 k(3), so k 2 and F(x) 2x.
(a) F(9) 2(9) 18N
(b) W 90
F(x) dx 90
2x dx x2 81 N cm30. F(x) kx; 10,000 k(1), so k 10,000.
(a) W d0
kx dx 12kx2 1
2kd2
1
2(10,000)(0.5)2
1250 inch-pounds
(b) For total distance: W 12(10,000)(1)2 5000
For second half of distance:
W 5000 1250 3750 inch-pounds
31.(1
2
2
(1
2)
0)[0.04 2(0.04) 2(0.05) 2(0.06) 2(0.05)
2(0.04) 2(0.04) 2(0.05) 2(0.04)
2(0.06) 2(0.06) 2(0.05) 0.05] 0.585
The overall rate, then, is0.
1
5
2
85 0.04875.
d
0
9
0
10.5
0.5
11
0
3
0
2
0
24
0
10
0
292 Section 7.1
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32.(1
2
2
(1
2)
0)[3.6 2(4.0) 2(3.1) 2(2.8) 2(2.8) 2(3.2)
2(3.3) 2(3.1) 2(3.2) 2(3.4) 2(3.4)
2(3.9) 4.0] 40 thousandths or 0.040
33. (a) x M
M
y . Taking dm dA as m
kand letting
dA 0, k yields .
(b) y M
M
y . Taking dm dA as m
kand letting
dA 0, k yields .
34. By symmetry, x 0. Fory, use horizontal strips:
y
1
5
2
35. By symmetry, y 0. Forx, use vertical strips:
x
4
3
s Section 7.2Areas in the Plane(pp. 374382)
Exploration 1 A Family of Butterflies
1. For k 1:
0
[(2 sinx) sinx] dx 0
(2 2 sinx) dx
2x 2 cosx 2 4
For k 2:
/20
[(4 2 sin 2x) (2 sin 2x)] dx
/20
(4 4 sin 2x) dx
4x 2 cos 2x 2 42. It appears that the areas for k 3 will continue to be
2 4.
3. Ak /k
0[(2k ksin kx) ksin kx] dx
/k0
(2k 2ksin kx) dx
If we make the substitution u kx, then du k dx and the
u-limits become 0 to . Thus,
Ak
/k0
(2k 2ksin kx) dx
/k0
(2 2 sin kx)k dx
0
(2 2 sin u) du.
4. 2 4
5. Because the amplitudes of the sine curves are k, the kth
butterfly stands 2kunits tall. The vertical edges alone have
lengths (2k) that increase without bound, so the perimeters
are tending to infinity.
Quick Review 7.2
1. 0
sinx dx cosx [1 1] 2
2. 10
e2x dx 12e2x 12(e2 1) 3.195
3. /4
/4
sec2x dx tanx 1 (1) 2
4. 20
(4x x3) dx 2x2 14x4 (8 4) 0 4
5. 33
9 x2 dx 9
2
(This is half the area of a circle of
radius 3.)
2
0
/4
/4
1
0
0
/2
0
0
2
3x320
x220
20
x(2x) dx
2
0 2x dx
x dA
dAx dA
dAx dm
dm
225y5/24
0
223y3/24
0
40
y(2 y) dy
40
2 y dy
y dA
dAy dA
dAy dm
dm
y dm
dm
mky
mk
x dm
dm
mkxk
mk
Section 7.2 293
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6. Solvex2 4x x 6.
x2 5x 6 0
(x 6)(x 1) 0
x 6 or x 1
y 6 6 12 or y 1 6 5
(6, 12) and (1, 5)
7. Solve ex x 1. From the graphs, it appears that ex is
always greater than or equal tox 1, so that if they are
ever equal, this is when ex (x 1) is at a minimum.
d
d
x[ex (x 1)] ex 1 is zero when ex 1, i.e., when
x 0. Test: e0 0 1 1. So the solution is (0, 1).
8. Inspection of the graphs shows two intersection points:
(0, 0), and (, 0). Check: 02 0 sin 0 0 and
2
2 sin 0.
9. Solvex2
2
x
1x3.
(0, 0) is a solution. Now divide byx.
x22
1x2
2 x4 x2
x4 x2 2 0
x2 1
2
1 8 2 or 1
Throw out the negative solution.
x 1
y x3 1
(0, 0), (1, 1) and (1, 1)
10. Use the intersect function on a graphing calculator:
[2, 2] by [2, 2]
(0.9286, 0.8008), (0, 0), and (0.9286, 0.8008)
Section 7.2 Exercises
1. 0
(1 cos2x) dx 12x 1
4 sin 2x 2
2. Use symmetry:
2/30
12 sec2 t 4 sin2 t dt /3
0
(sec2 t 8 sin2 t) dt
tan t 4t 2 sin 2t
3 43 3 0
4
3
3. 10
(y2 y3) dy 13y3
1
4y4 1
1
2
4. 10
[(12y2 12y3) (2y2 2y)] dy
10
(12y3 10y2 2y) dy
3y4
1
3
0y3 y2
3
1
3
0 1
4
3
5. Use the regions symmetry:
220
[2x2 (x4 2x2)] dx 220
(x4 4x2) dx
215x5 4
3x3
2352
3
3
2 0 11
2
5
8
6. Use the regions symmetry:
210
(x2 2x4) dx 213x3 2
5x5 213
2
5 21
2
5
7. Integrate with respect toy:
10
(2 y y) dy 43y3/2
1
2y2
43 1
2 0 56
8. Integrate with respect toy:
1
0[(2 y) y] dy
2y 12y2 2
3y3/2 2 12
2
3 0 56
9. Integrate in two parts:
02
[(2x3 x2 5x) (x2 3x)] dx
20
[(x2 3x) (2x3 x2 5x)] dx
02
(2x3 8x) dx 20
(2x3 8x) dx
1
2
x4 4x2
1
2
x4 4x2
[0 (8 16)] [(8 16) 0] 16
2
0
0
2
1
0
1
0
1
0
2
0
1
0
1
0
/3
0
0
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10. Integrate in three parts:
12
[(x 2) (4 x2)] dx
21
[(4 x2) (x 2)] dx
3
2[(x 2) (4 x2)] dx
12
(x2 x 2) dx 21
(x2 x 2) dx
32
(x2 x 2) dx
13x3 1
2x2 2x 13x
3
1
2x
2 2x
13x3
1
2x
2 2x
13 1
2 2 83 2 4
83 2 4 1
3
1
2 2
9 92 6 8
3 2 4
4
6
9 8
1
6
11. Solvex2 2 2: x2 4, so the curves intersect at
x 2.
22
[2 (x2 2)] dx 22
(4 x2) dx
4x 13x3 8 8
3 8 83
3
3
2 10
2
3
12. Solve 2x x2 3: x2 2x 3 (x 3)(x 1) 0,
so the curves intersect atx 1 andx 3.
31
(2x x2 3) dx x2 1
3x3 3x
(9 9 9) 1
1
3 3
3
3
2 10
2
3
13. Solve 7 2x2 x2 4: x2 1, so the curves intersect at
x 1.
11
[(7 2x2) (x2 4)] dx 11
(3x2 3) dx
311
(1 x2) dx
3 x 1
3x3
323 2
3 4
14.
[3, 3] by [1, 5]
The curves intersect atx 1 andx 2. Use the
regions symmetry:
210
[(x4 4x2 4)x2] dx 221
[x2 (x4 4x2 4)] dx
210
(x4 5x2 4) dx 221
(x4 5x2 4) dx
215x5 5
3x3 4x 215x5
5
3x3 4x
215 5
3 4 235
2
4
3
0 8 15
5
3 4 8
15.
32a, 3
2a by [a2, a2]
The curves intersect atx 0 andx a. Use the regions
symmetry:
2a0
x a2x2 dx 213(a2 x2)3/2 20 13a3
2
3a3
a
0
2
1
1
0
1
1
3
1
2
2
3
2
2
1
1
2
Section 7.2 295
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16.
[2, 12] by [0, 3.5]
The curves intersect at three points:
x 1, x 4 andx 9.
Because of the absolute value sign, break the integral up atx 0 also:
01x5
6 x dx
4
0x5
6 x dx
94 xx 5
6 dx
23(x)3/2 23x3/2
2
3x3/2
0 11
1
0
2
3 35
2
1
3
6 0
18 118
0
9 13
6
3
5
2
1
3
3
0
1
1
6
5
1
6
5
3 1
2
3
17.
[5, 5] by [1, 14]
The curves intersect atx 0 andx 4. Because of the
absolute value sign, break the integral up
atx 2 also (where x2 4 turns the corner). Use thegraphs symmetry:
220x2
2
4 (4 x2) dx 24
2x2
2
4 (x2 4) dx 22
0
3
2
x2 dx 24
2x2
2
8 dx 2
x
2
3
2
x
6
3
8x
2[4] 233
2 32 43 16
6
3
4 21
1
3
18. Solvey2 y 2: y2 y 2 (y 2)(y 1) 0, so the
curves intersect aty 1 andy 2.
21
(y 2 y2) dy 12y2 2y 1
3y3
2 4 83 1
2 2
1
3
92 41
2
19. Solve forx: x y
4
2
1 andx 4
y 4.
Now solve y
4
2
1 4
y 4:
y
4
2
4
y 5 0,
y2 y 20 (y 5)(y 4) 0.
The curves intersect aty 4 andy 5.
544
y 4 y4
2
1 dy
5
4y4
2
4y 5 dy
1y
2
3
y
8
2
5y
112
2
5
2
8
5 25 13
6 2 20 248
3 30
3
8
20. Solve forx: x y2 andx 3 2y2. Now solve
y2 3 2y2: y2 1, so the curves intersect at y 1.
Use the regions symmetry:
210
(3 2y2 y2) dy 210
(3 3y2) dy
610
(1 y2) dy
6 y 1
3y3
61 13 0 4
21. Solve forx: x y2 andx 2 3y2.
Now solve y2 2 3y2: y2 1, so the curves intersect
at y 1. Use the regions symmetry:
210
(2 3y2 y2) dy 210
(2 2y2) dy
410
(1 y2) dy 4 y 1
3y3 41 13 0
8
3
1
0
1
0
5
4
2
1
4
2
2
0
9
4
1
2x2 6x
5
4
0
1
2x2 6x
5
0
1
1
2x2 6x
5
296 Section 7.2
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22. Solve fory: y 4 4x2 andy x4 1.
Now solve 4 4x2 x4 1:
x4 4x2 5 (x2 1)(x2 5) 0.
The curves intersect at x = 1.
Use the regions symmetry:
210
[(4 4x2) (x4 1)] dx
210
(x4 4x2 5) dx
215x5 4
3x3 5x
215 4
3 5 0
1
1
0
5
4 6
1
1
4
5
23. Solve forx: x
3
y
2
andx
y
4
2
.
Now solve 3 y2 y
4
2
: y2 4,
so the curves intersect aty 2.
Use the regions symmetry:
220 3 y2 y4
2
dy 22
0 3 34y2 dy
23y y43
2(6 2) 0 8
24.
0
(2 sinx sin 2x) dx
2 cosx
1
2 cos 2x
2 12 2
1
2 4
25. Use the regions symmetry:
2 /30
(8 cosx sec2x) dx 28 sinx tanx 2[(4 3 3) 0] 6 3
26.
[1.1, 1.1] by [0.1, 1.1]
The curves intersect atx 0 andx 1, but they do not
cross atx 0.
2 10 1 x2 cos 2
x dx
2 x 1
3x3
2 sin 2
x
21 13 2 0 43
4 0.0601
27.
[1.5, 1.5] by [1.5, 1.5]
The curves intersect atx 0 andx 1. Use the areas
symmetry:
210sin 2
xx dx 2
2 cos 2
x 12x2
212 2
4
0.273
28. Use the regions symmetry, and simplify before integrating:
2 /40
(sec2x tan2x) dx
2 /40
[sec2x (sec2x 1)] dx
2 /40
dx 2 x 2
29. Use the regions symmetry:
2 /40
(tan2y tan2y) dy 4 /40
tan2y dy
4tany y 41 4 0
4 0.858
30. /20
3 siny cosy dy 323(cosy)3/2 30 23 2
31. Solve forx: x y3 andx y.
[1.5, 1.5] by [1.5, 1.5]
The curves intersect atx 0 andx 1. Use the areas
symmetry: 210
(y y3) dy 212y2 1
4y4 12
1
0
/2
0
/4
0
/4
0
1
0
1
0
/3
0
0
2
0
1
0
Section 7.2 297
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32.
[0.5, 2.5] by [0.5, 1.5]
y x andy
x
12 intersect atx 1. Integrate in two parts:
10
x dx 21
x
12 dx 12x2
1
x
1
2 12 (1) 1
33. The curves intersect when sinx cosx, i.e., atx
4.
/40
(cosx sinx) dx sinx cosx 2 1 0.414
34.
[3, 3] by [2, 4]
(a) The curves intersect atx 2.
Use the regions symmetry:
2 20
(3 x2 1) dx 2 20
(4 x2) dx
24x 13x3 28 83 0
3
3
2
(b) Solvey 3 x2 forx: x 3y. The
y-intercepts are 1 and 3.
31
2 3ydy 223(3 y)3/2
20 136 33
2
35. (a)
Ify x2 c, thenx c. So the points are
( c, c) and ( c, c).
(b) The two areas in Quadrant I, wherex y, are equal:
c0
y dy 4c
y dy
23y3/2 2
3y3/2
2
3c3/2
2
343/2
2
3c3/2
2c3/2
8
c3/2 4
c 42/3 24/3
(c) Divide the upper right section into a (4 c)-by- c
rectangle and a leftover portion:
c0
(c x2) dx (4 c) c 2 c
(4 x2) dx
cx 13x3
4 c c3/2 4x 13x
3
c3/2
1
3c3/2 4 c c3/2
8 83 4 c 1
3c3/2
2
3c3/2 4 c c3/2
1
3
6 4 c
1
3c3/2
4
3c3/2
1
3
6
c3/2 4
c 42/3 24/3
36.
[1, 5] by [1, 3]
The key intersection points are atx 0, x 1 andx 4.
Integrate in two parts:
101 x 4
x dx
4
1
2
x
4
x dx
x 2
3x3/2
x
8
2
4 x x82
1 23
1
8 (8 2) 4 18
1
3
1
4
1
1
0
2
c
c
0
4
c
c
0
y
5
x3
(c, c) (c, c)
y = 4(2, 4) (2, 4)
y = c
y =x2
3
1
2
0
/4
0
2
1
1
0
298 Section 7.2
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37. First find the two areas.
For the triangle, 1
2(2a)(a2) a3
For the parabola, 2a0
(a2 x2) dx 2a2x 13x3 4
3a3
The ratio, then, is 3
4, which remains
constant as a
approaches zero.
38. ba
[2f(x) f(x)] dx ba
f(x) dx, which we already know
equals 4.
39. Neither; both integrals come out as zero because the
1-to-0 and 0-to-1 portions of the integrals cancel each
other.
40. Sometimes true, namely when dA [f(x) g(x)] dx is
always nonnegative. This happens whenf(x) g(x) over
the entire interval.
41.
[1.5, 1.5] by [1.5, 1.5]
The curves intersect atx 0 andx 1. Use the areas
symmetry:
210x2
2
x
1 x3 dx 2ln x2 1 14x4
2 ln 2 1
2
ln 4 12 0.886
42.
[1.5, 1.5] by [1.5, 1.5]
The curves intersect atx 0 andx 0.9286. Use NINT
to find 20.92860
(sinx x3) dx 0.4303.
43. First graphy cosx andy x2.
[1.5, 1.5] by [0.5, 1.5]
The curves intersect atx 0.8241. Use NINT to find
20.82410
(cosx x2) dx 1.0948. Multiplying both
functions by kwill not change thex-value of any
intersection point, so the area condition to be met is
2 20.82410
(kcosx kx2) dx
2 k 20.82410
(cosx x2) dx
2 k(1.0948)
k 1.8269.
44. (a) Solve fory:
a
x2
2 b
y2
2 1
y2 b21 ax2
2y b1 ax
2
2
(b) aab1 ax
2
2 b1 ax2
2 dx or2aa
b1 ax2
2 dx or 4a
0b1 ax
2
2 dx
(c) Answers may vary.
(d, e) 2aa
b1 ax2
2 dx 2b2x1 ax
2
2 a
2 sin1
a
x
2ba2 sin1 (1) a
2 sin1 (1)
ab
45. By hypothesis, f(x) g(x) is the same for each region,
wheref(x) and g(x) represent the upper and lower edges.
But then Area
b
a [f
(x
) g
(x
)]dx
will be the same foreach.
a
a
1
0
a3
4
3a3
a
0
Section 7.2 299
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46. The curves are shown for m 1
2:
[1.5, 1.5] by [1,1]
In general, the intersection points are wherex2
x
1 mx,
which is wherex 0 or elsex m1 1. Then,because of symmetry, the area is
2 (1/m)10 x2
x
1 mx dx
212 ln (x2 1) 1
2mx2
ln m1 1 1
mm1
1 m ln (m) 1.
s Section 7.3Volumes(pp. 383394)
Exploration 1 Volume by Cylindrical Shells
1. Its height isf(xk) 3x
kx
k2.
2. Unrolling the cylinder, the circumference becomes one
dimension of a rectangle, and the height becomes the other.
The thickness x is the third dimension of a slab with
dimensions 2(xk 1) by 3x
kx
k2 by x. The volume is
obtained by multiplying the dimensions together.
3. The limit is the definite integral 3
0
2(x 1)(3x x2) dx.
4. 45
2
Exploration 2 Surface Area
1. ba
2y1 ddyx2
dxThe limit will exist iffandf are continuous on the interval
[a, b].
2. y sinx, so d
d
y
x cosx and
ba
2y1 ddyx2
dx
0
2 sin x 1cos2xdx 14.424.
3. y x, so d
d
y
x
2
1
x and
40
2 x1 21
x
2
dx 36.177.
Quick Review 7.3
1. x2
2. s
x
2, so Area s2
x
2
2
.
3. 1
2r2 or
2
x2
4. 1
2
d
2
2
or
8
x2
5. b x and h
2
3x, so Area
1
2bh
4
3x2.
6. b hx, so Area 1
2bh
x
2
2
.
7. b h
x
2, so Area
1
2bh
x
4
2
.
8.
b x and h (2x)2 12x2
2
15x, so
Area 1
2bh
4
15x2.
9. This is a 3-4-5 right triangle. b 4x, h 3x, and
Area 1
2bh 6x2.
10. The hexagon contains six equilateral triangles with sides of
lengthx, so from Exercise 5, Area 6 43x232
3x2.
Section 7.3 Exercises
1. In each case, the width of the cross section is
w 2 1x2.
(a) A r2, where r w
2, soA(x) w2
2 (1 x2).
(b) A s2, where s w, soA(x) w2 4(1 x2).
(c) A s2, where s
w
2
, soA(x)
w
2
2 2(1 x2).
(d) A
4
3w2 (see Quick Review Exercise 5), so
A(x)
4
3(2 1x2)2 3(1 x2).
2x2x
x
(1/m)1
0
300 Section 7.3
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2. In each case, the width of the cross section is w 2 x.
(a) A r2, where r w
2, so A(x) w2
2 x.
(b) A s2, where s w, soA(x) w2 4x.
(c) A s2, where s
w
2, soA(x)
w
2
2 2x.
(d) A
43w2 (see Quick Review Exercise 5), so
A(x)
4
3(2 x)2 3x.
3. A cross section has width w 2 x and area
A(x) s2
w
2
2 2x. The volume is
40
2x dx x2 16.
4. A cross section has width w (2x2)x2 2 2x2
and area A(x) r2
w
22
(1 x2
)2
. The volume is
11
(1 x2)2 dx 1
1
(x4 2x2 1) dx
15x5 2
3x3 x
1
1
6
5.
5. A cross section has width w 2 1x2 and area
A(x) s2 w2 4(1 x2). The volume is
11
4(1 x2) dx 411
(1 x2) dx 4 x 1
3x3 13
6.
6. A cross section has width w 2 1x2 and area
A(x) s2
w
2
2 2(1 x2). The volume is
11
2(1 x2) dx 211
(1 x2) dx 2 x 1
3x3 83.
7. A cross section has width w 2 sin x.
(a) A(x)
4
3w2 3 sinx, and
V 0
3 sinx dx
3
0
sinx dx
3cosx 2 3.
(b) A(x) s2 w2 4 sinx, and
V 0
4 sinx dx 40
sinx dx 4cosx 8.
8. A cross section has width w secx tanx.
(a) A(x) r2 w22
4(secx tanx)2, and
V /3/3
4(secx tanx)2 dx
4
/3
/3(sec2
x 2 secx tanx tan2
x) dx
4tanx 2 secx tanxx
2tanx secx 12x
2 3 2 6 3 2
6
3
6
2
.
(b) A(x) s2 w2 (secx tanx)2, and
V
/3
/3
(secx tanx)2 dx, which by same method as
in part (a) equals 4 3 2
3.
9. A cross section has width w 5y2 and area
r2 w22
5
4
y4. The volume is
20
5
4
y4 dy
4 y5 8.
10. A cross section has width w 2 1y2 and area
1
2s2
1
2w2 2(1 y2). The volume is
1
1
2(1 y2) dy 2y 13y3
83.11. (a) The volume is the same as if the square had moved
without twisting: VAh s2h.
(b) Still s2h: the lateral distribution of the square cross
sections doesnt affect the volume. Thats Cavalieris
Volume Theorem.
12. Since the diameter of the circular base of the solid extends
fromy 1
2
2 6 toy 12, for a diameter of 6 and a radius
of 3, the solid has the same cross sections as the right
circular cone. The volumes are equal by Cavalieris
Theorem.
13. The solid is a right circular cone of radius 1 and height 2.
V 1
3Bh
1
3(r2)h
1
3(12)2
2
3
14. The solid is a right circular cone of radius 3 and height 2.
V 1
3Bh
1
3(r2)h
1
3(32)2 6
1
1
2
0
/3
/3
/3
/3
0
0
1
1
1
1
1
1
4
0
Section 7.3 301
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15. A cross section has radius r tan 4y and areaA(y) r2 tan2 4y. The volume is10
tan2 4y dy 4 tan 4yy
4 1
4 .
16. A cross section has radius r sinx cosx and area
A(x) r2 sin2x cos2x. The shaded region extends
fromx 0 to where sinx cosx drops back to 0, i.e., where
x
2. Now, since cos 2x 2 cos2x 1, we know
cos2x 1 c
2
os 2x and since cos 2x 1 2 sin2x, we
know sin2x1 c
2
os 2x. /2
0 sin2x cos2x dx
/2
0
1 c2os 2x
1 c2os 2x
dx
4 /2
0(1 cos2 2x) dx
4 /2
0sin2 2x dx
4 /2
0
1 c
2
os 4x dx
8 /2
0(1 cos 4x) dx
8 x
1
4 sin 4x 8
2 0 0 16
2
.
17.
[2, 4] by [1, 5]
A cross section has radius rx2 and area
A(x) r2 x4. The volume is
20
x4 dx 15x5 32
5
.
18.
[4, 6] by [1, 9]
A cross section has radius rx3 and area
A(x) r2 x6. The volume is
20
x6 dx 17x7 12
7
8.
19.
[6, 6] by [4, 4]
The solid is a sphere of radius r 3. The volume is
43r3 36.
20.
[0.5, 1.5] by [0.5, 0.5]
The parabola crosses the liney 0 when
xx2 x(1 x) 0, i.e., whenx 0 orx 1. A cross
section has radius rxx2 and area
A(x)
r
2
(x
x
2
)
2
(x
2
2x
3
x
4
).The volume is
10
(x2 2x3 x4) dx 13x3 1
2x4
1
5x5 3
0.
21.
[1, 2] by [1, 2]
Use cylindrical shells: A shell has radiusy and heighty.
The volume is
1
0
2(y)(y) dy 213y3
23.22.
[1, 3] by [1, 3]
Use washer cross sections: A washer has inner radius rx,
outer radiusR 2x, and areaA(x) (R2 r2) 3x2.
The volume is 10
3x2 dx 3
1
3
x3
.
1
0
1
0
1
0
2
0
2
0
/2
0
1
0
302 Section 7.3
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23.
[2, 3] by [1, 6]
The curves intersect whenx2 1x 3, which is when
x2 x 2 (x 2)(x 1) 0, i.e., when
x 1 orx 2. Use washer cross sections: a washer hasinner radius rx2 1, outer radiusRx 3, and area
A(x) (R2 r2)
[(x 3)2 (x2 1)2]
(x4 x2 6x 8). The volume is
21
(x4 x2 6x 8) dx
15x5 1
3x3 3x2 8x
352
8
3 12 16 15
1
3 3 8 115
7.
24.
[2, 3] by [1, 5]
The curves intersect when 4 x2 2 x, which is when
x2 x 2 (x 2)(x 1) = 0, i.e., whenx1 or
x 2. Use washer cross sections: a washer has inner radius
r 2x, outer radiusR 4 x2, and area
A(x) (R2 r2)
[(4 x2)2 (2 x)2]
(12 4x 9x2 x4).
The volume is
2
1
(12 4x 9x2 x4) dx
12x 2x2 3x3 15x5
24 8 24 352 12 2 3 15
10
5
8.
25.
3,
3
by [0.5, 2]
Use washer cross sections: a washer has inner radius
r secx, outer radiusR 2, and areaA(x) (R2 r2) (2 sec2x).
The volume is
/4/4
(2 sec2x) dx 2x tanx
2 1
2 1
2 2.
26.
[1, 5] by [3, 1]
The curves intersect where x 2, which is wherex 4. Use washer cross sections: a washer has inner radius
r x, outer radiusR 2, and areaA(x) (R2 r2) (4 x).
The volume is 40
(4 x) dx 4x 12x2 827.
[0.5, 1.5] by [0.5, 2]
The curves intersect atx 0.7854. A cross section has
radius r 2 secx tanx and area
A(x) r2 ( 2 secx tanx)2. Use NINT to find
0.78540
( 2 secx tanx)2 dx 2.301.
28.
[1, 3] by [1, 3]
The curve and horizontal line intersect atx
2. A cross
section has radius 2 2 sinx and area
A(x) r2 4(1 sinx)2 4(1 2 sinx sin2x).
The volume is
/20
4(1 2 sinx sin2x) dx
432x 2 cosx 1
4sin 2x
434
2 (3 8)
29.
[1, 3] by [1.5, 1.5]
A cross section has radius r 5y2 and area
A(y) r2 5y4.
The volume is 11
5y4 dy y5 2.1
1
/2
0
4
0
/4
/4
2
1
2
1
Section 7.3 303
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30.
[1, 4] by [1, 3]
A cross section has radius ry3/2 and area
A(y) r2 y3. The volume is
20
y3 dy 14y4 4.31.
[1.2, 3.5] by [1, 2.1]
Use washer cross sections. A washer has inner radius r 1,
outer radiusRy 1, and area
A(y) (R2 r2) [(y 1)2 1] (y2 2y). The
volume is 10
(y2 2y) dy 13y3 y2 4
3.
32.
[1.7, 3] by [1, 2.1]
Use cylindrical shells: a shell has radiusx and heightx. The
volume is 10
2(x)(x) dx 2
1
3
x3
2
3
.
33.
[2, 4] by [1, 5]
Use cylindrical shells: A shell has radiusx and heightx2.
The volume is 20
2(x)(x2) dx 214x4 8.34.
[0.5, 1.5] by [0.5, 1.5]
The curves intersect atx 0 andx 1. Use cylindrical
shells: a shell has radiusx and height xx. The volume
is 10
2(x)( xx) dx 225x5/2 1
3x3 21
5.
35.
[1, 5] by [1, 3]
The curved and horizontal line intersect at (4, 2).
(a) Use washer cross sections: a washer has inner radius
r x, outer radiusR 2, and area
A(x) (R2 r2) (4 x). The volume is
40(4x) dx 4x 12x2 8
(b) A cross section has radius ry2 and area
A(y) r2 y4.
The volume is 20
y4 dy 15y5 32
5
.
(c) A cross section has radius r 2 x and area
A(x) r2 (2 x)2 (4 4 xx).
The volume is
40
(4 4 xx) dx 4x 83x3/2 1
2x2 83
.
(d) Use washer cross sections: a washer has inner radius
r 4 y2, outer radiusR 4, and area
A(y) (R2 r2) [16 (4 y2)2]
(8y2 y4).
The volume is
20(8y2 y4) dy 83y3
1
5y5 221
4
5
36.
[1, 3] by [1, 3]
The slanted and vertical lines intersect at (1, 2)
(a) The solid is a right circular cone of radius 1 and
height 2. The volume is
1
3Bh
1
3(r2)h
1
3(12)2
2
3.
(b) Use cylindrical shells: a shell has radius 2x and
height 2x. The volume is
10
2(2 x)(2x) dx 41
0
(2xx2) dx
4 x2 1
3x3 83
.1
0
2
0
4
0
2
0
4
0
1
0
2
0
1
0
1
0
2
0
304 Section 7.3
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37.
[2, 2] by [1, 2]
The curves intersect at (1, 1).
(a) A cross section has radius r 1x2
and area
A(x) r2 (1 x2)2 (1 2x2 x4).
The volume is
11
(1 2x2 x4) dx x 2
3x3
1
5x5 11
6
5
.
(b) Use cylindrical shells: a shell has radius 2y and
height 2 y. The volume is
10
2(2 y)(2 y) dy 41
0
(2 yy3/2) dy
443y3/2 2
5y5/2 51
6
5
.
(c) Use cylindrical shells: a shell has radiusy 1 and
height 2 y. The volume is
10
2(y 1)(2 y) dy 41
0
(y3/2 y) dy
425y5/2 2
3y3/2 61
4
5
.
38. (a) A cross section has radius r h1 bx and area
A(x) r2 h21 bx
2. The volume is
b
0h
2
1b
x
2
dx h2
b
31 b
x
3
3bh2
.
(b) Use cylindrical shells: a shell has radiusx and height
h1 bx. The volume is
b0
2(x)h1 bx dx 2h
b
0x xb
2
dx 2h12x2 3
x
b
3
3b2h.
39.
[2, 3] by [2, 3]
A shell has radiusx and heightx 2x 32x.
The volume is 20
2(x)32x dx x3 8.
40.
[2, 2] by [1, 3]
x2 2 x atx 1. A shell has radiusx and height
2 xx2. The volume is
10
2(x)(2 xx2) dx 2x2 1
3x3
1
4x4 56
.
41.
[1, 5] by [1, 3]
A shell has radiusx and height x. The volume is
40
2(x)( x) dx 225x5/2 12
5
8.
42.
[2, 2] by [2, 2]
The functions intersect where 2x 1 x, i.e., atx 1.
A shell has radiusx and height
x (2x 1) x 2x 1. The volume is
10
2(x)( x 2x 1) dx 21
0
(x3/2 2x2 x) dx
225x5/2 2
3x3
1
2x2
7
1
5.
43. A shell has height 12(y2 y3).
(a) A shell has radiusy. The volume is
10
2(y)12(y2 y3) dy 241
0
(y3 y4) dy
2414y4 1
5y5 65
.
(b) A shell has radius 1y. The volume is
1
0
2(1 y)12(y2 y3) dy
241
0
(y4 2y3 y2) dy
2415y5 1
2y4
1
3y3 45
.1
0
1
0
1
0
4
0
1
0
2
0
b
0
b
0
1
0
1
0
1
1
Section 7.3 305
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43. continued
(c) A shell has radius 8
5y. The volume is
10
285y12(y2 y3) dy 24
1
0y4 15
3y3
8
5y2 dy
24
1
5
y5 1
2
3
0
y4
1
8
5
y3
2.
(d) A shell has radiusy 2
5. The volume is
10
2y 2512(y2 y3) dy 24
1
0y4 5
3y3
2
5y2 dx
2415y5 23
0y4
1
2
5y3 2.
44. A shell has height y
2
2
y44
y
2
2
y2 y44
.
(a) A shell has radiusy. The volume is
20
2(y)y2 y44
dy 214y4 21
4y6 83
.
(b) A shell has radius 2 y. The volume is
20
2(2y)y2 y44
dy 2
2
0 y4
5
y
2
4
y3 2y2 dy 22
1
4y6
1
1
0y5
1
4y4
2
3y3 85
.
(c) A shell has radius 5y. The volume is
20
2(5y)y2 y44
dy 2
2
0y4
5
5
4
y4y3 5y2 dy
221
4y6
1
4y5
1
4y4
5
3y3 8.
(d) A shell has radiusy 5
8. The volume is
20
2y 58y2 y
4
4
dy
2
2
0 y
4
5
5
3
y
2
4
y3
5
8
y2
dy 22
1
4y6
3
1
2y5
1
4y4
2
5
4y3 4.
45.
[1, 3] by [1.4, 9.1]
The functions intersect at (2, 8).
(a) Use washer cross sections: a washer has inner radius
rx3, outer radiusR 4x, and area
A(x) (R2 r2) (16x2 x6). The volume is
20
(16x2 x6) dx 136x3
1
7x7 512
2
1
.
(b) Use cylindrical shells: a shell has a radius 8y and
heighty1/3 4
y. The volume is
80
2(8 y)y1/3 4y dy
2
8
0
8y1/3 2yy4/3
y
4
2
dy
26y4/3 y2 37y7/3 11
2y3 832
2
1
.
46.
[0.5, 1.5] by [0.5, 1.5]
The functions intersect at (0, 0) and (1, 1).
(a) Use cylindrical shells: a shell has radiusx and height
2x
x
2
x
x
x
2
. The volume is
10
2(x)(xx2) dx 213x3 1
4x4 6.
(b) Use cylindrical shells: a shell has radius 1x and
height 2xx2 xx x2. The volume is
10
2(1 x)(xx2) dx 21
0
(x3 2x2 x) dx
214x4 2
3x3
1
2x2
6.
1
0
1
0
8
0
2
0
2
0
2
0
2
0
2
0
1
0
1
0
306 Section 7.3
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47.
[0.5, 2.5] by [0.5, 2.5]
The intersection points are 14, 1, 1
4, 2, and (1, 1).
(a) A washer has inner radius r 14, outer radiusR
y12,
and area (R2 r2) y14 1
1
6. The volume is
21
y14 1
1
6 dy 3
1
y3
1
1
6y 14
1
8
.
(b) A shell has radiusx and height
1
x 1. The volume is
11/4
2(x)
1
x 1 dx 223x3/2
1
2x2 14
1
8
.
48. (a) For 0 x , x f(x) x(si
x
n x) sinx.
Forx 0, x f(x) 0 1 sin 0 sinx. So
x f(x) sinx for 0 x .
(b) Use cylindrical shells: a shell has radiusx and heighty.
The volume is 0
2xy dx, which from part (a) is
0
2 sinx dx 2cosx 4.
49. (a) A cross section has radius r 1
x
2 36x2 and area
A(x) r2 1
44(36x2 x4). The volume is
6
0
1
44(36x2 x4) dx
1
4412x
3 15x5 365
cm3.
(b) 365
cm3(8.5 g/cm3) 192.3 g
50. A cross section has radius r c sinx and area
A(x) r2 (c sinx)2 (c2 2c sinx sin2x).
The volume is
0
(c2 2c sinx sin2x) dx
c2x 2c cosx
1
2x 1
4sin 2x c2 2c 12 2c
2c2 4c
2
2
.
(a) Solve
d
d
c2c2 4c 2
2
022c 4 0
c 2 0
c
2
This value ofc gives a minimum for Vbecause
a
d
2
c
V
2 22 0.
Then the volume is 2
2
2 4
2 2
2
2
2
4
(b) Since the derivative with respect to c is not zero
anywhere else besides c
2, the maximum must occur
at c 0 or c 1. The volume for c 0 is
2
2
4.935,
and for c 1 it is(3
2
8) 2.238. c 0
maximizes the volume.
(c)
[0, 2] by [0, 6]
The volume gets large without limit. This makes sense,
since the curve is sweeping out space in an
ever-increasing radius.
51. (a) Using d C
, andA d22
4
C
2
yields the
following areas (in square inches, rounded to the
nearest tenth): 2.3, 1.6, 1.5, 2.1, 3.2, 4.8, 7.0, 9.3, 10.7,
10.7, 9.3, 6.4, 3.2.
(b) IfC(y) is the circumference as a function ofy, then the
area of a cross section is
A(y) C(y2)/
2
C
4
2
(y),
and the volume is 4
1
60
C2(y) dy.
(c) 4
1
60
A(y) dy 4
1
60
C2(y) dy
4
1
6 2
4
0[5.42 2(4.52 4.42
5.12 6.32 7.82 9.42 10.82 11.62
11.62 10.82 9.02) 6.32] 34.7 in.3
0
6
0
0
1
1/4
2
1
Section 7.3 307
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52. (a) A cross section has radius r 2y and area
r2 2y. The volume is 50
2y dy y2 25.
(b) V(h) A(h) dh, so d
d
V
hA(h).
d
d
V
t
d
d
V
h
d
d
h
tA(h)
d
d
h
t,
so d
d
h
t
A(
1
h)
d
d
V
t
For h 4, the area is 2(4) 8,
so d
d
h
t
8
1
3un
se
it
c
s3 =
8
3
un
se
it
c
s3.
53. (a)
The remaining solid is that swept out by the shaded
region in revolution. Use cylindrical shells: a shell has
radiusx and height 2 r2x2. The volume is
..
2(x)(2 r2x2) dx
223(r2 x2)3/2
4
3
(
8)
32
3
.
(b) The answer is independent ofr.
54. Partition the appropriate interval in the axis of revolution
and measure the radius r(x) of the shadow region at these
points. Then use an approximation such as the trapezoidal
rule to estimate the integral ba
r2(x) dx.
55. Solve axx2 0: This is true atx 0 andx a. For
revolution about thex-axis, a cross section has radius
r axx2 and area
A(x) r2 (axx2)2 (a2x2 2ax3 x4).
The volume is
a
0
(a2x2 2ax3 x4) dx 13a2x3 1
2ax4
1
5x5
3
1
0a5.
For revolution about they-axis, a cylindrical shell has
radiusx and height axx2. The volume is
a0
2(x)(axx2) dx 213ax3 1
4x4 16a4.
Setting the two volumes equal,
3
1
0a5
1
6a4 yields
3
1
0a
1
6, so a 5.
56. The slant height s of a tiny horizontal slice can be
written as s x2y2 1(g(y))2y. So the
surface area is approximated by the Riemann sum
n
k1
2g(yk) 1(g(y))2y. The limit of that is the
integral.
57. g(y) ddxy
21
y
, and
20
2 y1 21
y
2
dy 2
0
4y1dy
6(4y 1)3/2
13
3
13.614
58. g(y) d
d
x
yy2, and
10
2y33
1(y2)2dy 231
6(1 y4)3/2
9(2 2 1) 0.638.
59. g(y) d
d
x
y
1
2y1/2 , and
31
2 y1/2 133/2
1 12y1/22
dy
23
1
y1/2 133/2
1 41y dy.Using NINT, this evaluates to 16.110
1
0
2
0
a
0
a
0
r
r24
r
r222
y
2
2
x
r
5
0
308 Section 7.3
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60. g(y) d
d
x
y 2y
1
1, and
15/8
2 2y11 2y1
12
dy
21
5/8
2y dy
2 223y3/2
4
3
21 1
5
652 2.997.
61. f(x) d
d
y
x 2x, and
20
2x2 1(2x)2 dx 20
2x2 14x2dx evaluates,
using NINT, to 53.226.
62. f(x)
d
d
y
x 3 2x, and
30
2(3xx2) 1(32x)2 dx evaluates, using NINT,
to 44.877.
63. f(x) d
d
y
x
1
2x
x
x2, and
1.50.5
2 2xx21 1
2x
x
x22
dx 21.5
0.5
1 dx
2 x 2 6.283
64. f(x) d
d
y
x
2 x
1
1, and
51
2 x11 2x1
12
dx
25
1 x 5
4 dx
223x 5
4
3/2
4
3
2
4
5
3/2
9
4
3/2
49
3
51.313
65. Hemisphere cross sectional area: ( R2h2)2 A1.
Right circular cylinder with cone removed cross sectional
area: R2 h2 A2
SinceA1A
2, the two volumes are equal by Cavalieris
theorem. Thus, volume of hemisphere
volume of cylinder volume of cone
R3 1
3R3
2
3R3.
66. Use washer cross sections: a washer has inner radius
r b a2y2, outer radiusR b a2y2, and
area (R2 r2)
[(b a2y2)2 (b a2y2)2]
4b a2y2. The volume is
a
a
4b a2y2 dy 4ba
a
a2y2 dy
4b2a2
22a2b
67. (a) Put the bottom of the bowl at (0, a). The area of a
horizontal cross section is ( a2y2)2 (a2 y2).
The volume for height h is
haa
(a2 y2) dy a2y 13y3 h2(3
3
a h).
(b) For h 4, y 1 and the area of a cross section is
(52 12) 24. The rate of rise is
d
d
h
t
A
1
d
d
V
t
24
1
(0.2)12
1
0 m/sec.
68. (a) A cross section has radius r a2x2 and area
A(x) r2 ( a2x2)2 (a2 x2). The
volume is
a
a
(a2 x2) dx
a2x
1
3
x3
a3 13a3 a3
1
3a3
4
3a3.
(b) A cross section has radiusx r1 hy and area
A(y) x2 r21 hy
2 r21 2h
y
h
y2
2. Thevolume is
h0
r21 2hy
h
y2
2 dy r2 y yh2
3
y
h
3
2
1
3r2h.
h
0
a
a
ha
a
5
1
1.5
0.5
1
5/8
Section 7.3 309
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s Section 7.4 Lengths of Curves(pp. 395401)
Quick Review 7.4
1. 12xx2 (1x)2, which, sincex 1, equals1 x orx 1.
2.
1x
x
42
1 2
x
2
, which, sincex 2, equals1
2
x or
2
2
x.
3. 1(tan x)2 (secx)2, which, since 0 x
2,
equals secx.
4. 1 4x 1x2
12 116x2 x12 14(x2
x
24
)2 which,
sincex 0, equalsx2
4
x
4.
5. 1cos2x 2 cos2x, which, since
2 x
2,
equals 2 cosx.
6. f(x) has a corner atx 4.
7. d
d
x(5x2/3)
3
1
3
0
x is undefined atx 0.f(x) has a cusp
there.
8. d
d
x(
5
x3)5(x
1
3)4/5 is undefined forx 3.
f(x) has a vertical tangent there.
9. x24x4 x 2 has a corner atx 2.
10. d
d
x1
3
sin x3(sc
i
o
n
s
x
x
)2/3 is undefined forx k,
where kis any integer.f(x) has vertical tangents at these
values ofx.
Section 7.4 Exercises
1. (a) y 2x, so
Length 21
1(2x)2 dx 21
14x2dx.
(b)
[
1, 2] by [
1, 5](c) Length 6.126
2. (a) y sec2x, so Length 0/3
1sec4x dx.
(b)
3, 0 by [3, 1](c) Length 2.057
3. (a) x cosy, so Length 0
1cos2ydy.
(b)
[1, 2] by [1, 4]
(c) Length 3.820
4. (a) x y(1 y2)1/2, so
Length 1/21/211
y
2
y2 dy.(b)
[1, 2] by [1, 1]
(c) Length 1.047
5. (a) y2 2y 2x 1, so
y2 2y 1 (y 1)2 2x 2, and
y 2x2 1. Theny 2x
1
2, and
Length 711 2x1 2 dx.
(b)
[1, 7] by [2, 4]
(c) Length 9.2946. (a) y cosxx sinx cosxx sinx, so
Length 0
1x2sin2x dx.
(b)
[0, ] by [1, 4]
(c) Length 4.698
7. (a) y tanx, so Length /60
1tan2x dx.
(b) y tanx dx ln (secx)
0, 6 by [0.1, 0.2](c) Length 0.549
310 Section 7.4
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8. (a) x sec2y1, so Length /4/3
secy dy.
(b) x sec2y1 tany,
sox
[2.4, 2.4] by 2,
2
(c) Length 2.198
9. (a) y secx tanx, so
Length /3/3
1 sec2xtan2x dx.
(b)
3,
3 by [1, 3]
(c) Length 3.139
10. y (ex
2
ex), so Length 3
31 ex
2e
x
2
dx.(b)
[3, 3] by [2, 12]
(c) Length 20.036
11. y 1
2(x2 2)1/2(2x) x x22, so the length is
30
1 (xx22)2 dx 30
x42x21dx
30
(x2 1) dx 13x3 x 12.
12. y 3
2 x, so the length is
401 32x
2
dx 4
0 1 94x dx
28
71 9
4
x
3/2
80
2
1
7
0 8.
13. x y2 4
1
y2, so the length is 3
1 1 y2 41y22
dy 3
1 y2 41y22
dy 13y3 41
y 56
3.
14. x y3 4
1
y3, so the length is
21 1 y3 41y3
2
dy 2
1 y3 41y32
dy
14y4 81y2
1
3
2
2
3.
15. x y
2
2
2
1
y2, so the length is
21 1 y2
2
21y22
dy 2
1 y22
21
y22
dy
16y3 21
y 11
7
2.
16. y
x2
2x
1
(4x
4
4)2
(x
1)
2
4(x
1
1)2
so the length is
20 1 (x 1)24(x
1 1)2
2
dx
20 (x 1)24(x
1 1)2
2
dx
13(x 1)3 4(x1
1) 56
3.
2
0
2
1
2
1
3
1
4
0
3
0
3 y 0
0 y
4
ln (cosy)
ln (cosy)
Section 7.4 311
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25/35
17. x sec4y1, so the length is
/4/4
1 (sec4y1) dy /4/4
sec2y dy
tany 2.
18. y 3x41, so the length is
1
2
1 (3x41) dx 1
2
3x2 dx
313x3 7
3
3.
19. (a) ddy
x
2corresponds to
4
1
x here, so take
d
d
y
x as
2
1
x. Then
y x C, and, since (1, 1) lies on the curve, C 0.
Soy x.
(b) Only one. We know the derivative of the function and
the value of the function at one value ofx.
20. (a)
d
d
x
y
2
corresponds to
y
1
4
here, so take
d
d
x
y
as
y
1
2
.
Thenx 1
y Cand, since (0, 1) lies on the curve,
C 1. Soy 1
1
x.
(b) Only one. We know the derivative of the function and
the value of the function at one value ofx.
21. y cos2x, so the length is
/40
1 cos2x dx /40
2 cos2xdx
2sinx 1.
22. y (1 x2/3)1/2x1/3, so the length is
81 2/4 1 (1 x2/3)x2/3 dx
81 24 x2/3 dx
81 2/4
x1/3 dx
832x2/3
832 3
212 6.
23. Find the length of the curvey sin 3
2
0x for 0 x 20.
y 3
2
0 cos
3
2
0x, so the length is
200 1 32
0 cos
3
2
0x
2
dx, which evaluates, using NINT,
to 21.07 inches.
24. The area is 300 times the length of the arch.
y 2 sin
50
x, so the length is
25251
2
2
sin250x dx, which evaluates, using NINT,
to 73.185. Multiply that by 300, then by $1.75 to obtain
the cost (rounded to the nearest dollar): $38,422.
25. For track 1: y1
0 atx 10 5 22.3607, and
y1
10
0
0
.2x
0.2x2. NINT fails to evaluate
10 510 5
1 (y1
)2 dx because of the undefined slope at
the limits, so use the tracks symmetry, and back away
from the upper limit a little, and find
2
22.36
0
1
(
y1
)2
dx 52.548. Then, pretending the lastlittle stretch at each end is a straight line, add
2 100 0.2(22.36)2 0.156 to get the total length of
track 1 as 52.704. Using a similar strategy, find the
length of the right halfof track 2 to be 32.274. Now
enter Y1
52.704 and
Y2
32.274 + NINT1 15
00
.2
t
0.2t22
, t, x, 0 andgraph in a [30, 0] by [0, 60] window to see the effect of
thex-coordinate of the lane-2 starting position on the length
of lane 2. (Be patient!) Solve graphically to find the
intersection atx 19.909, which leads to starting point
coordinates (19.909, 8.410).
26. f(x) 1
3x2/3
2
3x1/3, but NINT fails on
20
1 (f(x))2 dx because of the undefined slope at
x 0. So, instead solve forx in terms ofy using the
quadratic formula. (x1/3)2 x1/3 y 0, and
x1/3 1
2
1 4y. Using the positive values,
x 1
8( 1 4y 1)3. Then,
x 3
8( 1 4y 1)2
1
2
4y, and
21/3 2
2/3
0
1 (x)2dy 3.6142.
1
2/4
/4
0
1
2
/4
/4
312 Section 7.4
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26/35
27. f(x) , so the
length is 11/21
2
dx which evaluates,
using NINT, to 2.1089.
28. There is a corner atx 0:
[2, 2] by [1, 5]
Break the function into two smooth segments:
y and
y .
The length is 12
1 (y)2dy
02
1 (3x25)2dx 10
1 (3x25)2dx,
which evaluates, using NINT for each part, to 13.132.
29. y (1 x)2, 0 x 1
[0.5, 2.5] by [0.5, 1.5]
y
x x
1, but NINT may fail usingy over the entire
interval becausey is undefined atx 0. So, split the curve
into two equal segments by solving x y 1 with
y x: x 1
4. The total length is 21
1/41 xx 12
dx,which evaluates, using NINT, to 1.623.
30.
[0, 16] by [0, 2]
y 1
4x3/4, but NINT may fail usingy over the entire
interval, becausey is undefined atx 0. So, use
x y4, 0 y 2: x 4y3 and the length is
20
1 (4y3)2dy, which evaluates,
using NINT, to 16.647.
31. Because the limit of the sum xkas the norm of the
partition goes to zero will always be the length (b a) of
the interval (a, b).
32. No; the curve can be indefinitely long. Consider, for
example, the curve 1
3
sin
1
x
+ 0.5 for 0 x 1.
33. (a) The fin is the hypotenuse of a right triangle with leg
lengths xk
and d
d
x
fxxk1xkf(xk1)xk.
(b) limnn
k1
(xk
)2(f(xk
1)x
k)2
limnn
k1
xk 1 (f(x
k
1))2
ba
1 (f(x))2 dx
34. Yes. Any curve of the formy x c, where c is a
constant, has constant slope 1, so that
a0
1 (y)2dx a0
2 dx a 2.
s Section 7.5Applications from Scienceand Statistics(pp. 401411)
Quick Review 7.5
1. (a) 10
ex dx ex 1 1e(b) 0.632
2. (a) 10
ex dx ex e 1(b) 1.718
3. (a) /2/4
sinx dx cosx 22
(b) 0.707
4. (a) 30
(x2 2) dx 13x3 2x 15(b) 15
5. (a)
2
1x3
x
2
1dx 13 ln (x
3 1)
1
3[ln 9 ln 2]
1
3ln 92
(b) 0.501
6. 70
2(x 2) sinx dx
7. 70
(1 x2)(2x) dx
2
1
3
0
/2
/4
1
0
1
0
2 x 0
0 x 1
3x2 5
3x2 5
2 x 0
0 x 1
x3 5x
x3 5x
4x2 8x 1
(4x2 1)2
4x2 8x 1
(4x 1)2(4x2 1) (8x2 8x)
(4x2 1)2
Section 7.5 313
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27/35
8. 70
cos2x dx
9. 70
2y
2(10 y) dy
10. 70
4
3 sin2x dx
Section 7.5 Exercises
1. 50
xex/3 dx 3ex/3(3 x) e25
4/3 9 4.4670 J
2. 30
x sin 4x dx
4
4 sin 4
x x cos 4
x
4
2
2
3
2
3.8473 J
3. 30
x 9 x2 dx 13(9 x2)3/2 9 J
4.
10
0 (esinx
cosx 2) dx esinx
2x esin 10 19 19.5804 J
5. When the bucket isx m off the ground, the water weighs
F(x) 490202
0
x 4901 2
x
0 490 24.5x N.
Then
W 200
(490 24.5x) dx 490x 12.25x2 4900 J.6. When the bucket isx m off the ground, the water weighs
F(x) 49020 204x/5 4901 2
x
5 490 19.6x N.
Then
W 200
(490 19.6x) dx 490x 9.8x2 5880 J.7. When the bag isx ft off the ground, the sand weighs
F(x) 14418 18x/2 1441 3
x
6 144 4x lb.
Then
W 180
(144 4x) dx 144x 2x2 1944 ft-lb8. (a) F ks, so 800 k(14 10) and k 200 lb/in.
(b) F(x) 200x, and 20
200x dx
100x2
400 in.-lb.
(c) F 200s, so s 1
2
6
0
0
0
0 8 in.
9. (a) F ks, so 21,714 k(8 5) and k 7238 lb/in.
(b) F(x) 7238x. W 1/20
7238x dx 3619x2 904.75 905 in.-lb, and W 1
1/2
7238x dx
3619x2 2714.25 2714 in.-lb.
10. (a) F ks, so 150 k11
6 and k 2400 lb/in. Then for
s 1
8, F 240018 300 lb.
(b) 1/80
2400x dx 1200x2 18.75 in.-lb
11. When the end of the rope is x m from its starting point, the
(50 x) m of rope still to go weigh
F(x) (0.624)(50 x) N. The total work is
500
(0.624)(50 x) dx 0.62450x 12x2 780 J.
12. (a) Work (p2, V2)(p
1, V
1)
F(x) dx (p2, V2)(p
1, V
1)
pA dx (p2, V2)(p
1, V
1)
p dV
(b) p1V
11.4
(50)(243)1.4 109,350, so p 10
V
91
,3.4
50 and
Work (p2, V2)
(p1, V
1)
10V9
1,3.450
dV
109,3502.5V0.4 37,968.75 in.-lb
13. (a) From the equationx2 y2 32, it follows that a thin
horizontal rectangle has area 2 9 y2 y, wherey is
distance from the top, and pressure 62.4y. The total
force is approximatelyn
k1
(62.4yk
)(2 9 yk
2) y
n
k1
124.8yk 9 y
k2y.
(b) 30
124.8y 9 y2 dy 41.6(9 y2)3/2 1123.2 lb
14. (a) From the equation 3
x2
2 8
y2
2 1, it follows that a thin
horizontal rectangle has area 61 6y42
y, wherey isdistance from the top, and pressure 62.4y. The total
force is approximately
n
k1
(62.4yk)61
y
6k42
y n
k1
374.4yk1
y
6k42
y.
(b) 80
374.4y1 6y42
dy 7987.21 6y
4
2
3/2
7987.2 lb
8
0
3
0
V 32
V 243
50
0
1/8
0
1
1/2
1/2
0
2
0
18
0
20
0
20
0
10
0
3
0
3
0
5
0
314 Section 7.5
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28/35
15. (a) From the equationx 3
8y, it follows that a thin
horizontal rectangle has area 3
4yy, wherey is the
distance from the top of the triangle, the pressure is
62.4(y 3). The total force is approximately
n
k
1
62.4(yk 3)34yk y
n
k
1
46.8(yk2 3y
k) y.
(b) 83
46.8(y22 3y) dy 15.6y3 70.2y2
3494.4 (210.6) 3705 lb
16. (a) From the equationy x
2
2
, it follows that a thin
horizontal rectangle has area 2 2yy, wherey is
distance from the bottom, and pressure 62.4(4y).
The total force is approximately
n
k1
62.4(4 yk)(2 2y
k)y
n
k1124.8 2(4 yk
yk3/2
)y.
(b) 40
124.8 2(4 yy3/2) dy
124.8 283y3/2 2
5y5/2
1064.96 2 1506.1 lb
17. (a) Work to raise a thin slice 62.4(10 12)(y)y.
Total work 200
62.4(120)y dy 62.460y2 1,497,600 ft-lb
(b) (1,497,600 ft-lb) (250 ft-lb/sec) 5990.4 sec
100 min
(c) Work to empty half the tank 100
62.4(120)y dy
62.460y2 374,400 ft-lb, and374,400 250 1497.6 sec 25 min
(d) The weight per ft3 of water is a simple multiplicative
factor in the answers. So divide by 62.4 and multiply
by the appropriate weight-density
For 62.26:
1,497,600662
2
.
.
2
4
6 1,494,240 ft-lb and
5990.4662
2
.
.
2
4
6 5976.96 sec 100 min.
For 62.5:
1,497,600662
2
.
.
5
4 1,500,000 ft-lb and
5990.4662
2
.
.
5
4 6000 sec 100 min.
18. The work needed to raise a thin disk is (10)2(51.2)yy,
wherey is height up from the bottom. The total work is
300
100(51.2)y dy 512012y2 7,238,229 ft-lb
19. Work to pump through the valve is (2)2(62.4)(y 15)y
for a thin disk and
60
4(62.4)(y 15) dy 249.612y2 15y 84,687.3 ft-lb
for the whole tank. Work to pump over the rim is
(2)2(62.4)(6 15)y for a thin disk and
60
4(62.4)(21) dy 4(62.4)(21)(6) 98,801.8 ft-lb for
the whole tank. Through a hose attached to a valve in the
bottom is faster, because it takes more time for a pump with
a given power output to do more work.
20. The work is the same as if the straw were initially an inch
long and just touched the surface, and lengthened as the
liquid level dropped. For a thin disk, the volume is
y1417.5
2y and the work to raise it is
y1417.5
2
49(8y)y. The total work is
7
0
y
14
17.5
2
4
9
(8
y) dy, which using NINT evaluates
to 91.3244 in.-oz.
21. The work is that already calculated (to pump the oil to the
rim) plus the work needed to raise the entire amount 3 ft
higher. The latter comes to
13r2h(57)(3) 57(4)2(8) 22,921.06 ft-lb, and thetotal is 22,921.06 30,561.41 53,482.5 ft-lb.
22. The weight density is a simple multiplicative factor: Divide
by 57 and multiply by 64.5.
30,561.416547.5 34,582.65 ft-lb.
6
0
30
0
10
0
20
0
4
0
8
3
Section 7.5 315
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29/35
23. The work to raise a thin disk is
r2(56)h ( 102y2)2(56)(10 2 y)y
56(12 y)(100 y2)y. The total work is
100
56(12 y)(100 y2) dy, which evaluates using NINT
to 967,611 ft-lb. This will come to
(967,611)($0.005) $4838, so yes, theres enough moneyto hire the firm.
24. Pipe radius 1
6 ft;
Work to fill pipe 3600
162(62.4)y dy 112,320 ft-lb.
Work to fill tank 385360
(10)2(62.4)y dy
58,110,000ft-lb.
Total work 58,222,320 ft-lb, which will take
58,222,320 1650 110,855 sec 31 hr.
25. (a) The pressure at depthy is 62.4y, and the area of a thin
horizontal strip is 2y. The depth of water is 1
6
1 ft, so
the total force on an end is
11/60
(62.4y)(2 dy) 209.73 lb.
(b) On the sides, which are twice as long as the ends, the
initial total force is doubled to 419.47 lb. When the
tank is upended, the depth is doubled to 1
3
1 ft, and the
force on a side becomes 11/30
(62.4y)(2 dy) 838.93 lb,
which means that the fluid force doubles.
26. 3.75 in. 1
5
6 ft, and 7.75 in.
3
4
1
8 ft.
Force on a side p dA 31/480
(64.5y)156 dy 4.2 lb.27. (a) 0.5 (50%), since half of a normal distribution lies
below the mean.
(b) Use NINT to find
65
63f(x) dx, where
f(x) 3.2
1
2e(x63.4)
2/(2 3.2
2). The result is
0.24 (24%).
(c) 6 ft 72 in. Pick 82 in. as a conveniently high upper
limit and with NINT, find 8272
f(x) dx. The result is
0.0036 (0.36%).
(d) 0 if we assume a continuous distribution. Between
59.5 in. and 60.5 in., the proportion is
60.559.5
f(x) dx 0.071 (7.1%)
28. Usef(x) 100
1
2e(x498)
2/(2 1002)
(a)
500
400f(x) dx 0.34 (34%)
(b) Take 1000 as a conveniently high upper limit:
1000700
f(x) dx 0.217, which means about
0.217(300) 6.5 people
29. Integration is a good approximation to the area (which
represents the probability), since the area is a kind of
Riemann sum.
30. The proportion of lightbulbs that last between 100 and 800
hours.
31.
35,780,000
6,370,000 100
r02MG
dr 1000MG
1
r
, which for
M 5.975 1024, G 6.6726 1011 evaluates to
5.1446 1010 J.
32. (a) The distance goes from 2 m to 1 m. The work by an
external force equals the work done by repulsion in
moving the electrons from a 1-m distance to a 2-m
distance:
Work 2
1
23 r120
29
dr
23 10291r 1.15 1028 J
(b) Again, find the work done by the fixed electrons in
pushing the third one away. The total work is the sum
of the work by each fixed electron. The changes in
distance are 4 m to 6 m and 2 m to 4 m, respectively.
Work 64
23
r
12
029 dr 4
2
23
r
12
029 dr
23 1029
1
r
1
r
7.6667 1029 J.
4
2
6
4
2
1
35,780,000
6,370,000
316 Section 7.5
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30/35
33. F mddvt mvddvx, soW x2
x1
F(x) dx
x2x
1
mvddvx dx v2
v
1
mv dv
1
2mv
22
1
2mv
12
34. Work Change in kinetic energy 1
2mv2.
m32
2
ft
o
/s
z
ec2
32
1/
f
8
t/s
l
e
b
c2
2
1
56 slug, so
Work 1
22
1
56(160)2 50 ft-lb.
35. 0.3125 lb 3
0
2
.31
ft
2
/s
5
ec
lb2 0.009765625 slug, and
90 mph 905218
m
0
i
ft36
1
00
hr
sec 132 ft/sec, so
Work change in kinetic energy 12(0.009765625)(132)2
85.1 ft-lb.
36. 1.6 oz 1.6 oz116lobz/(32 ft/sec2) 0.003125 slug, soWork
1
2(0.003125)(280)2 122.5 ft-lb.
37. 2 oz 2 oz116lobz/(32 ft/sec2) 2156 slug, and124 mph 124 mph521
8
m
0
i
ft36
1
00
hr
sec 181.867 ft/sec,
so Work 1
22
1
56(181.867)2 64.6 ft-lb.
38. 14.5 oz 14.5 oz11
6
l
o
b
z/(32 ft/sec2) 0.02832 slug, so
Work 1
2(0.02832)(88)2 109.7 ft-lb.
39. 6.5 oz 6.5 oz11
6
l
o
b
z/(32 ft/sec2) 0.01270 slug, so
Work 1
2(0.01270)(132)2 110.6 ft-lb.
40. 2 oz 1
8 lb
2
1
56 slug. Compression energy of spring
1
2ks2
1
2(18)14
2 0.5625 ft-lb, and final height is
given by mgh 0.5625 ft-lb, so h
(1/
0
2
.
5
5
6
6
)
2
(
5
32)
4.5 ft.
s Chapter 7 Review Exercises
(pp. 413415)
1. 50
v(t) dt 50
(t2 0.2t3) dt
13t3 0.05t4 10.417 ft
2.
7
0 c(t) dt 7
0 (4 0.001t4
) dt
4t 0.0002t5 31.361 gal
3. 1000
B(x) dx 1000
(21 e0.03x) dx
21x 33.333e0.03x 1464
4. 20
(x) dx 20
(11 4x) dx 11x 2x2 14 g
5.
24
0 E(t) dt
24
0 3002
cos
1
2
t
dt
3002t 12 sin 12t 14,4006.
[1, 3] by [1, 2]
The curves intersect atx 1. The area is
1
0
x dx 2
1
x12 dx
12x2
1x
1
2 12 1 1.
7.
[4, 4] by [4, 4]
The curves intersect atx 2 andx 1. The area is
1
2
[3 x2 (x 1)] dx 1
2
(x2 x 2) dx
13x3 12x2 2x
13 12 2 83 2 4
9
2.
1
2
2
1
1
0
24
0
2
0
100
0
7
0
5
0
Chapter 7 Review 317
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31/35
8. x y 1 impliesy (1 x)2 1 2 xx.
[0.5, 2] by [0.5, 1]
The area is
1
0(1 2 xx) dx
x 43x3/2 1
2x2
1
6.
9. x 2y2 impliesy 2x.
[1, 19] by [1, 4]
The curves intersect atx 18. The area is
180 3 2
x dx 3x 432x
3/2
18,or 3
02y2 dy 23y3 18.
10. 4xy2 4 impliesx 1
4y2 1, and 4xy 16 implies
x 1
4y 4.
[6, 6] by [6, 6]
The curves intersect at (3, 4) and (5.25, 5). The area is
54
1
4y 4 14y2 1 dy
54
1
4y2
1
4y 5 dy
112y3 18y2 5y
4
2
2
4
5 338 2483 30.375.
11.
[0.1, 1] by [0.1, 1]
The area is /40
(x sinx) dx 12x2 cosx
32
2
2
2 1
0.0155.
12.
2, 3
2
by [3,3]
The area is
0
(2 sinx sin 2x) dx 2 cosx 12 cos 2x 4.13.
[5, 5] by [5, 5]
The curves intersect atx 2.1281. The area is
2.12812.1281
(4x2 cosx) dx,
which using NINT evaluates to 8.9023.
14.
[4, 4] by [4, 4]
The curves intersect atx 0.8256. The area is
0.82560.8256
(3 x sec2x) dx,
which using NINT evaluates to 2.1043.
15. Solve 1 cosx 2 cosx for thex-values at the two
ends of the region: x 2
3, i.e.,
5
3
or
7
3
. Use the
symmetry of the area:
27/32
[(1 cosx) (2 cosx)] dx
27/32
(2 cosx 1) dx
22 sinxx 2 3
2
3 1.370.
16. 5/3
/3
[(2 cosx) (1 cosx)] dx
5/3/3
(1 2 cosx) dx
x 2 sinx 2 3
4
3 7.653
5/3
/3
7/3
2
0
/4
0
5
4
3
0
18
0
1
0
318 Chapter 7 Review
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32/35
17. Solvex3 x x2
x
1 to find the intersection points at
x 0 andx 21/4. Then use the areas symmetry:
the area is
221/4
0 x2 x
1 (x3 x) dx
2
12 ln (x2 1) 14x
4 12x2
ln ( 2 1) 2 1 1.2956.
18. Use the intersect function on a graphing calculator to
determine that the curves intersect atx 1.8933.
The area is
1.89331.893331x
2
x2
1
0
3 dx,
which using NINT evaluates to 5.7312.
19. Use thex- andy-axis symmetries of the area:
40
x sinx dx 4sinx x cosx 4.20. A cross section has radius r 3x4 and area
A(x) r2 9x8.
V 11
9x8 dx x9 2.21.
[5, 5] by [5, 5]
The graphs intersect at (0, 0) and (4, 4).
(a) Use cylindrical shells. A shell has radiusy and height
y y
4
2
. The total volume is
40
2(y) y y42
dy 24
0 y2 y
4
3
dy 213y3 116y4
32
3
.
(b) Use cylindrical shells. A shell has radiusx and height
2 xx. The total volume is
40
2(x)(2 xx) dx 24
0
(2x3/2 x2) dx
245x5/2 13x3
12
1
8
5
.
(c) Use cylindrical shells. A shell has radius 4 x and
height 2 xx. The total volume is
40
2(4 x)(2 xx) dx
24
0
(8 x 4x 2x3/2 x2) dx
2136x3/2 2x2 45x5/2 13x3 645.
(d) Use cylindrical shells. A shell has radius 4 y and
heighty y
4
2
. The total volume is
40
2(4 y)y y42
dy 2
4
0 4y 2y2 y
4
3
dy 22y2 23y3 116y4 323.
22. (a) Use disks. The volume is
2
0 ( 2y)2 dy
2
0 2y dy y2 4.
(b) k
02y dy y2 k2
(c) Since V k2, d
d
V
t 2k
d
d
k
t.
When k 1, d
d
k
t
2
1
k
d
d
V
t 2
1
(2)
1,
so the depth is increasing at the rate of
1 unit per
second.
23. The football is a solid of revolution about thex-axis. A
cross section has radius 121 142x12
and arear2 121 142x1
2
. The volume is, given the symmetry,211/2
0
121 142x12
dx 2411/2
0 1 14
2
x
1
2
dx 24x 121
2
13x3 24121 161 88 276 in3.
24. The width of a cross section is 2 sinx, and the area is
1
2r2
1
2 sin2x. The volume is
0
1
2 sin2x dx
212x 14sin 2x 4
2
.
0
11/2
0
k
0
2
0
4
0
4
0
4
0
4
0
1
1
0
21/4
0
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25.
[1, 2] by [1, 2]
Use washer cross sections. A washer has inner radius r 1,
outer radiusR ex/2, and area (R2 r2) (ex 1).
The volume is
ln 30
(ex 1) dx ex x (3 ln 3 1)
(2 ln 3).
26. Use cylindrical shells. Taking the hole to be vertical, a shell
has radiusx and height 2 22x2. The volume of the
piece cut out is
3
0
2(x)(2 22x2) dx 2 3
0
2x 4x2 dx
223(4 x2)3/2
4
3(1 8)
28
3
29.3215 ft3.
27. The curve crosses thex-axis atx 3.y 2x, so the
length is 33
1(2x)2 dx 33
14x2dx, which
using NINT evaluates to 19.4942.
28.
[2, 2] by [2, 2]
The curves intersect atx 0 andx 1. Use the graphs
x- andy-axis symmetry:
d
d
x(x3 x) 3x2 1, and the total perimeter is
4
1
0
1(3x21)2dx, which using NINT evaluates to
5.2454.
29.
[1, 3] by [3, 3]
y 3x2 6x equals zero whenx 0 or 2. The maximum
is atx 0, the minimum at x = 2. The distance between
them along the curve is 20
1(3x26x)2 dx, which
using NINT evaluates to 4.5920. The time taken is about
4.5
2
920 2.296 sec.
30. If (b) were true, then the curvey ksinx would have to
get vanishingly short as kapproached zero. Since in fact the
curves length approaches 2 instead, (b) is false and (a) is
true.
31. F(x) x41, so
5
2 1(F(x))2dx
5
2 x4dx
52
x2 dx
13x3 39.32. (a) (100 N)(40 m) = 4000 J
(b) When the end has traveled a distancey, the weight of
the remaining portion is (40 y)(0.8) 32 0.8y.
The total work to lift the rope is
40
0
(32 0.8y) dy
32y 0.4y2
640 J.
(c) 4000 640 4640 J
33. The weight of the water at elevationx (starting fromx 0)
is (800)(8)47540750x/2 192584750 12x. The total workis 4750
0
1
9
2
5
84750 12x dx 192584750x 14x2
22,800,000 ft-lb.
34. F ks, so k Fs
08.03 80
30 N/m. Then
Work 0.30
80
3
0x dx 806
0x2 12 J.
To stretch the additional meter,
Work 1.30.3
80
3
0x dx 806
0x2 213.3 J.
35. The work is positive going uphill, since the force pushes in
the direction of travel. The work is negative going downhill.
1.3
0.3
0.3
0
4750
0
40
0
5
2
3
0
ln 3
0
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36. The radius of a horizontal cross section is 82y2, where
y is distance below the rim. The area is (64 y2), the
weight is 0.04(64 y2) y, and the work to lift it over
the rim is 0.04(64 y2)(y) y. The total work is
82
0.04y(64 y2) dy 0.048
2
(64y y3) dy
0.0432y2 14y4 36 113.097 in.-lb.
37. The width of a thin horizontal strip is