chapter 04
TRANSCRIPT
January 27, 2005 11:44 L24-ch04 Sheet number 1 Page number 127 black
127
CHAPTER 4
Derivatives of Logarithmic, Exponential, andInverse Trigonometric Functions
EXERCISE SET 4.1
1. y = (2x− 5)1/3; dy/dx =23(2x− 5)−2/3
2. dy/dx =13[2 + tan(x2)
]−2/3sec2(x2)(2x) =
23x sec2(x2)
[2 + tan(x2)
]−2/3
3. dy/dx =23
(x+ 1x− 2
)−1/3x− 2− (x+ 1)
(x− 2)2= − 2
(x+ 1)1/3(x− 2)5/3
4. dy/dx =12
[x2 + 1x2 − 5
]−1/2d
dx
[x2 + 1x2 − 5
]=
12
[x2 + 1x2 − 5
]−1/2 −12x(x2 − 5)2
= − 6x(x2 − 5)3/2
√x2 + 1
5. dy/dx = x3(−23
)(5x2 + 1)−5/3(10x) + 3x2(5x2 + 1)−2/3 =
13x2(5x2 + 1)−5/3(25x2 + 9)
6. dy/dx = −3√2x− 1x2 +
1x
23(2x− 1)2/3
=−4x+ 3
3x2(2x− 1)2/3
7. dy/dx =52[sin(3/x)]3/2[cos(3/x)](−3/x2) = −15[sin(3/x)]3/2 cos(3/x)
2x2
8. dy/dx = −12[cos(x3)
]−3/2 [− sin(x3)](3x2) =
32x2 sin(x3)
[cos(x3)
]−3/2
9. (a) 1 + y + xdy
dx− 6x2 = 0,
dy
dx=
6x2 − y − 1x
(b) y =2 + 2x3 − x
x=
2x+ 2x2 − 1,
dy
dx= − 2
x2 + 4x
(c) From Part (a),dy
dx= 6x− 1
x− 1xy = 6x− 1
x− 1x
(2x+ 2x2 − 1
)= 4x− 2
x2
10. (a)12y−1/2 dy
dx− cosx = 0 or
dy
dx= 2√y cosx
(b) y = (2 + sinx)2 = 4 + 4 sinx+ sin2 x sody
dx= 4 cosx+ 2 sinx cosx
(c) from Part (a),dy
dx= 2√y cosx = 2 cosx(2 + sinx) = 4 cosx+ 2 sinx cosx
11. 2x+ 2ydy
dx= 0 so
dy
dx= −x
y
12. 3x2 + 3y2 dy
dx= 3y2 + 6xy
dy
dx,dy
dx=
3y2 − 3x3y2 − 6xy
=y2 − x2
y2 − 2xy
13. x2 dy
dx+ 2xy + 3x(3y2)
dy
dx+ 3y3 − 1 = 0
(x2 + 9xy2)dy
dx= 1− 2xy − 3y3 so
dy
dx=
1− 2xy − 3y3
x2 + 9xy2
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128 Chapter 4
14. x3(2y)dy
dx+ 3x2y2 − 5x2 dy
dx− 10xy + 1 = 0
(2x3y − 5x2)dy
dx= 10xy − 3x2y2 − 1 so
dy
dx=
10xy − 3x2y2 − 12x3y − 5x2
15. − 12x3/2 −
dydx
2y3/2 = 0,dy
dx= −y
3/2
x3/2
16. 2x =(x− y)(1 + dy/dx)− (x+ y)(1− dy/dx)
(x− y)2,
2x(x− y)2 = −2y + 2xdy
dxso
dy
dx=
x(x− y)2 + y
x
17. cos(x2y2)[x2(2y)
dy
dx+ 2xy2
]= 1,
dy
dx=
1− 2xy2 cos(x2y2)2x2y cos(x2y2)
18. − sin(xy2)[y2 + 2xy
dy
dx
]=
dy
dx,dy
dx= − y2 sin(xy2)
2xy sin(xy2) + 1
19. 3 tan2(xy2 + y) sec2(xy2 + y)(2xy
dy
dx+ y2 +
dy
dx
)= 1
sody
dx=
1− 3y2 tan2(xy2 + y) sec2(xy2 + y)3(2xy + 1) tan2(xy2 + y) sec2(xy2 + y)
20.(1 + sec y)[3xy2(dy/dx) + y3]− xy3(sec y tan y)(dy/dx)
(1 + sec y)2= 4y3 dy
dx,
multiply through by (1 + sec y)2 and solve fordy
dxto get
dy
dx=
y(1 + sec y)4y(1 + sec y)2 − 3x(1 + sec y) + xy sec y tan y
21. 4x− 6ydy
dx= 0,
dy
dx=
2x3y
, 4− 6(dy
dx
)2
− 6yd2y
dx2 = 0,
d2y
dx2 = −3(dydx
)2− 2
3y=
2(3y2 − 2x2)9y3 = − 8
9y3
22.dy
dx= −x
2
y2 ,d2y
dx2 = −y2(2x)− x2(2ydy/dx)
y4 = −2xy2 − 2x2y(−x2/y2)y4 = −2x(y3 + x3)
y5 ,
but x3 + y3 = 1 sod2y
dx2 = −2xy5
23.dy
dx= −y
x,d2y
dx2 = −x(dy/dx)− y(1)x2 = −x(−y/x)− y
x2 =2yx2
24. y + xdy
dx+ 2y
dy
dx= 0,
dy
dx= − y
x+ 2y, 2
dy
dx+ x
d2y
dx2 + 2(dy
dx
)2
+ 2yd2y
dx2 = 0,d2y
dx2 =2y(x+ y)(x+ 2y)3
25.dy
dx= (1 + cos y)−1,
d2y
dx2 = −(1 + cos y)−2(− sin y)dy
dx=
sin y(1 + cos y)3
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Exercise Set 4.1 129
26.dy
dx=
cos y1 + x sin y
,
d2y
dx2 =(1 + x sin y)(− sin y)(dy/dx)− (cos y)[(x cos y)(dy/dx) + sin y]
(1 + x sin y)2
= −2 sin y cos y + (x cos y)(2 sin2 y + cos2 y)(1 + x sin y)3
,
but x cos y = y, 2 sin y cos y = sin 2y, and sin2 y + cos2 y = 1 so
d2y
dx2 = − sin 2y + y(sin2 y + 1)(1 + x sin y)3
27. By implicit differentiation, 2x + 2y(dy/dx) = 0,dy
dx= −x
y; at (1/2,
√3/2),
dy
dx= −
√3/3; at
(1/2,−√3/2),
dy
dx= +
√3/3. Directly, at the upper point y =
√1− x2,
dy
dx=
−x√1− x2
=
− 1/2√3/4
= −1/√3 and at the lower point y = −
√1− x2,
dy
dx=
x√1− x2
= +1/√3.
28. If y2 − x + 1 = 0, then y =√x− 1 goes through the point (10, 3) so dy/dx = 1/(2
√x− 1). By
implicit differentiation dy/dx = 1/(2y). In both cases, dy/dx|(10,3) = 1/6. Similarly y = −√x− 1
goes through (10,−3) so dy/dx = −1/(2√x− 1) = −1/6 which yields dy/dx = 1/(2y) = −1/6.
29. 4x3 + 4y3 dy
dx= 0, so
dy
dx= −x
3
y3 = − 1153/4 ≈ −0.1312.
30. 3y2 dy
dx+ x2 dy
dx+ 2xy + 2x− 6y
dy
dx= 0, so
dy
dx= −2x y + 1
3y2 + x2 − 6y= 0 at x = 0
31. 4(x2 + y2)(2x+ 2y
dy
dx
)= 25
(2x− 2y
dy
dx
),
dy
dx=
x[25− 4(x2 + y2)]y[25 + 4(x2 + y2)]
; at (3, 1)dy
dx= −9/13
32.23
(x−1/3 + y−1/3 dy
dx
)= 0,
dy
dx= −y
1/3
x1/3 =√3 at (−1, 3
√3)
33. 4a3 da
dt− 4t3 = 6
(a2 + 2at
da
dt
), solve for
da
dtto get
da
dt=
2t3 + 3a2
2a3 − 6at
34.12u−1/2 du
dv+
12v−1/2 = 0 so
du
dv= −√u√v
35. 2a2ωdω
dλ+ 2b2λ = 0 so
dω
dλ= − b2λ
a2ω36. 1 = (cosx)
dx
dyso
dx
dy=
1cosx
= secx
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130 Chapter 4
37. (a)
–4 4
–2
2
x
y
(b) Implicit differentiation of the equation of the curve yields (4y3 + 2y)dy
dx= 2x− 1 so
dy
dx= 0
only if x = 1/2 but y4 + y2 ≥ 0, so x = 1/2 is impossible.
(c) x2 − x− (y4 + y2) = 0, so by the Quadratic Formula x =1±
√1 + 4y2 + 4y4
2= 1 + y2,−y2
which gives the parabolas x = 1 + y2, x = −y2.
38. (a) y
–2
0
2
1 2
x
(b) 2ydy
dx= (x − a)(x − b) + x(x − b) + x(x − a) = 3x2 − 2(a + b)x + ab. If
dy
dx= 0 then
3x2 − 2(a+ b)x+ ab = 0. By the Quadratic Formula
x =2(a+ b)±
√4(a+ b)2 − 4 · 3ab6
=13
[a+ b± (a2 + b2 − ab)1/2
].
(c) y = ±√x(x− a)(x− b). The square root is only defined for nonnegative arguments, so it is
necessary that all three of the factors x, x− a, x− b be nonnegative, or that two of them benonpositive. If, for example, 0 < a < b then the function is defined on the disjoint intervals0 < x < a and b < x < +∞, so there are two parts.
39. (a) y
x
2
–2 2
–2
(b) x ≈ ±1.1547
(c) Implicit differentiation yields 2x− xdy
dx− y + 2y
dy
dx= 0. Solve for
dy
dx=
y − 2x2y − x
. Ifdy
dx= 0
then y − 2x = 0 or y = 2x. Thus 4 = x2 − xy + y2 = x2 − 2x2 + 4x2 = 3x2, x = ± 2√3.
40. (a) See Exercise 39 (a)(b) Since the equation is symmetric in x and y, we obtain, as in Exercise 39, x ≈ ±1.1547.
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Exercise Set 4.1 131
(c) Implicit differentiation yields 2x− xdy
dx− y + 2y
dy
dx= 0. Solve for
dx
dy=
2y − x
y − 2x. If
dx
dy= 0
then 2y − x = 0 or x = 2y. Thus 4 = 4y2 − 2y2 + y2 = 3y2, y = ± 2√3, x = 2y = ± 4√
3.
41. Solve the simultaneous equations y = x, x2−xy+y2 = 4 to get x2−x2+x2 = 4, x = ±2, y = x = ±2,so the points of intersection are (2, 2) and (−2,−2).From Exercise 39 part (c),
dy
dx=
y − 2x2y − x
. When x = y = 2,dy
dx= −1; when x = y = −2, dy
dx= −1;
the slopes are equal.
42. Suppose a2 − 2ab+ b2 = 4. Then (−a)2 − 2(−a)(−b) + (−b)2 = a2 − 2ab+ b2 = 4 so if P (a, b) lieson C then so does Q(−a,−b).
From Exercise 39 part (c),dy
dx=
y − 2x2y − x
. When x = a, y = b thendy
dx=
b− 2a2b− a
, and when
x = −a, y = −b, then dy
dx=
b− 2a2b− a
, so the slopes at P and Q are equal.
43. The point (1,1) is on the graph, so 1 + a = b. The slope of the tangent line at (1,1) is −4/3; use
implicit differentiation to getdy
dx= − 2xy
x2 + 2ayso at (1,1), − 2
1 + 2a= −4
3, 1 + 2a = 3/2, a = 1/4
and hence b = 1 + 1/4 = 5/4.
44. The slope of the line x + 2y − 2 = 0 is m1 = −1/2, so the line perpendicular has slope m = 2(negative reciprocal). The slope of the curve y3 = 2x2 can be obtained by implicit differentiation:
3y2 dy
dx= 4x,
dy
dx=
4x3y2 . Set
dy
dx= 2;
4x3y2 = 2, x = (3/2)y2. Use this in the equation of the curve:
y3 = 2x2 = 2((3/2)y2)2 = (9/2)y4, y = 2/9, x =32
(29
)2
=227
.
45. (a)
–3 –1 2
–3
–1
2
x
y (b) x ≈ 0.84
(c) Use implicit differentiation to get dy/dx = (2y−3x2)/(3y2−2x), so dy/dx = 0 if y = (3/2)x2.Substitute this into x3 − 2xy + y3 = 0 to obtain 27x6 − 16x3 = 0, x3 = 16/27, x = 24/3/3and hence y = 25/3/3.
46. (a)
–3 –1 2
–3
–1
2
x
y (b) Evidently the tangent line at the pointx = 1, y = 1 has slope −1.
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132 Chapter 4
(c) Use implicit differentiation to get dy/dx = (2y−3x2)/(3y2−2x), so dy/dx = −1 if 2y−3x2 =−3y2+2x, 2(y−x)+3(y−x)(y+x) = 0. One solution is y = x; this together with x3+y3 = 2xyyields x = y = 1. For these values dy/dx = −1, so that (1, 1) is a solution.
To prove that there is no other solution, suppose y = x. From dy/dx = −1 it followsthat 2(y − x) + 3(y − x)(y + x) = 0. But y = x, so x + y = −2/3. Then x3 + y3 =(x + y)(x2 − xy + y2) = 2xy, so replacing x + y with −2/3 we get x2 + 2xy + y2 = 0, or(x+y)2 = 0, so y = −x. Substitute that into x3 +y3 = 2xy to obtain x3−x3 = −2x2, x = 0.But at x = y = 0 the derivative is not defined.
47. (a) The curve is the circle (x − 2)2 + y2 = 1 about the point (2, 0) of radius 1. One tangentline is tangent at a point P(x,y) in the first quadrant. Let Q(2, 0) be the center of thecircle. Then OPQ is a right angle, with sides |PQ| = r = 1 and |OP | =
√x2 + y2. By
the Pythagorean Theorem x2 + y2 + 12 = 22. Substitute this into (x − 2)2 + y2 = 1 toobtain 3 − 4x + 4 = 1, x = 3/2, y =
√3− x2 =
√3/2. So the required tangent lines are
y = ±(√3/3)x.
(b) Let P (x0, y0) be a point where a line through the origin is tangent to the curvex2 − 4x+ y2 + 3 = 0. Implicit differentiation applied to the equation of the curve givesdy/dx = (2− x)/y. At P the slope of the curve must equal the slope of the line so(2− x0)/y0 = y0/x0, or y2
0 = 2x0 − x20. But x
20 − 4x0 + y2
0 + 3 = 0 because (x0, y0) is on thecurve, and elimination of y2
0 in the latter two equations gives x20 − 4x0 + (2x0 − x2
0) + 3 = 0,x0 = 3/2 which when substituted into y2
0 = 2x0 − x20 yields y2
0 = 3/4, so y0 = ±√3/2. The
slopes of the lines are (±√3/2)/(3/2) = ±
√3/3 and their equations are y = (
√3/3)x and
y = −(√3/3)x.
48. Let P (x0, y0) be a point where a line through the origin is tangent to the curve2x2 − 4x+ y2 + 1 = 0. Implicit differentiation applied to the equation of the curve givesdy/dx = (2− 2x)/y. At P the slope of the curve must equal the slope of the line so(2− 2x0)/y0 = y0/x0, or y2
0 = 2x0(1− x0). But 2x20 − 4x0 + y2
0 + 1 = 0 because (x0, y0) is on thecurve, and elimination of y2
0 in the latter two equations gives 2x0 = 4x0− 1, x0 = 1/2 which whensubstituted into y2
0 = 2x0(1 − x0) yields y20 = 1/2, so y0 = ±
√2/2. The slopes of the lines are
(±√2/2)/(1/2) = ±
√2 and their equations are y =
√2x and y = −
√2x.
49. The linear equation axr−10 x+ byr−1
0 y = c is the equation of a line �. Implicit differentiation of the
equation of the curve yields raxr−1+rbyr−1 dy
dx= 0,
dy
dx= −ax
r−1
byr−1 . At the point (x0, y0) the slope
of the line must be −axr−10
byr−10
, which is the slope of �. Moreover, the equation of � is satisfied by
the point (x0, y0), so this point lies on �. By the point-slope formula, � must be the line tangentto the curve at (x0, y0).
50. Implicit differentiation of the equation of the curve yields rxr−1+ryr−1 dy
dx= 0. At the point (1, 1)
this becomes r + rdy
dx= 0,
dy
dx= −1.
51. By the chain rule,dy
dx=
dy
dt
dt
dx. Use implicit differentiation on 2y3t+ t3y = 1 to get
dy
dt= −2y3 + 3t2y
6ty2 + t3, but
dt
dx=
1cos t
sody
dx= − 2y3 + 3t2y
(6ty2 + t3) cos t.
52. (a) f ′(x) =43x1/3, f ′′(x) =
49x−2/3
(b) f ′(x) =73x4/3, f ′′(x) =
289x1/3, f ′′′(x) =
2827x−2/3
(c) generalize parts (a) and (b) with k = (n− 1) + 1/3 = n− 2/3
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Exercise Set 4.2 133
53. y′ = rxr−1, y′′ = r(r − 1)xr−2 so 3x2[r(r − 1)xr−2
]+ 4x
(rxr−1
)− 2xr = 0,
3r(r − 1)xr + 4rxr − 2xr = 0, (3r2 + r − 2)xr = 0,3r2 + r − 2 = 0, (3r − 2)(r + 1) = 0; r = −1, 2/3
54. y′ = rxr−1, y′′ = r(r − 1)xr−2 so 16x2[r(r − 1)xr−2
]+ 24x
(rxr−1
)+ xr = 0,
16r(r − 1)xr + 24rxr + xr = 0, (16r2 + 8r + 1)xr = 0,16r2 + 8r + 1 = 0, (4r + 1)2 = 0; r = −1/4
55. We shall find when the curves intersect and check that the slopes are negative reciprocals. For theintersection solve the simultaneous equations x2 + (y − c)2 = c2 and (x− k)2 + y2 = k2 to obtain
cy = kx =12(x2 + y2). Thus x2 + y2 = cy + kx, or y2 − cy = −x2 + kx, and
y − c
x= −x− k
y.
Differentiating the two families yields (black)dy
dx= − x
y − c, and (gray)
dy
dx= −x− k
y. But it was
proven that these quantities are negative reciprocals of each other.
56. Differentiating, we get the equations (black) xdy
dx+ y = 0 and (gray) 2x − 2y
dy
dx= 0. The first
says the (black) slope is = −yx
and the second says the (gray) slope isx
y, and these are negative
reciprocals of each other.
EXERCISE SET 4.2
1.15x
(5) =1x
2.1x/3
13=
1x
3.1
1 + x4.
12 +√x
(1
2√x
)=
12√x(2 +
√x)
5.1
x2 − 1(2x) =
2xx2 − 1
6.3x2 − 14x
x3 − 7x2 − 3
7.1
x/(1 + x2)
[(1 + x2)(1)− x(2x)
(1 + x2)2
]=
1− x2
x(1 + x2)
8.1
(1 + x)/(1− x)1− x+ 1 + x
(1− x)2=
21− x2 9.
d
dx(2 lnx) = 2
d
dxlnx =
2x
10. 3 (lnx)21x
11.12(lnx)−1/2
(1x
)=
12x√lnx
12.1√x
12√x=
12x
13. lnx+ x1x= 1 + lnx
14. x3(1x
)+ (3x2) lnx = x2(1 + 3 lnx) 15. 2x log2(3− 2x)− 2x2
(3− 2x) ln 2
16.[log2(x2 − 2x)
]3 + 3x[log2(x2 − 2x)
]2 2x− 2(x2 − 2x) ln 2
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134 Chapter 4
17.2x(1 + log x)− x/(ln 10)
(1 + log x)218. 1/[x(ln 10)(1 + log x)2]
19.1
lnx
(1x
)=
1x lnx
20.1
ln(ln(x))1
lnx1x
21.1
tanx(sec2 x) = secx cscx 22.
1cosx
(− sinx) = − tanx
23. − 1xsin(lnx) 24. 2 sin(lnx) cos(lnx)
1x=
sin(2 lnx)x
=sin(lnx2)
x
25.1
ln 10 sin2 x(2 sinx cosx) = 2
cotxln 10
26.1
(ln 10)(1− sin2 x)(−2 sinx cosx) = − 2 sinx cosx
(ln 10) cos2 x= −2 tanx
ln 10
27.d
dx
[3 ln(x− 1) + 4 ln(x2 + 1)
]=
3x− 1
+8x
x2 + 1=
11x2 − 8x+ 3(x− 1)(x2 + 1)
28.d
dx[2 ln cosx+
12ln(1 + x4)] = −2 tanx+
2x3
1 + x4
29.d
dx
[ln cosx− 1
2ln(4− 3x2)
]= − tanx+
3x4− 3x2
30.d
dx
(12[ln(x− 1)− ln(x+ 1)]
)=
12
(1
x− 1− 1x+ 1
)
31. ln |y| = ln |x|+ 13ln |1 + x2|, dy
dx= x
3√1 + x2
[1x+
2x3(1 + x2)
]
32. ln |y| = 15[ln |x− 1| − ln |x+ 1|], dy
dx=
15
5
√x− 1x+ 1
[1
x− 1− 1x+ 1
]
33. ln |y| = 13ln |x2 − 8|+ 1
2ln |x3 + 1| − ln |x6 − 7x+ 5|
dy
dx=
(x2 − 8)1/3√x3 + 1
x6 − 7x+ 5
[2x
3(x2 − 8)+
3x2
2(x3 + 1)− 6x5 − 7x6 − 7x+ 5
]
34. ln |y| = ln | sinx|+ ln | cosx|+ 3 ln | tanx| − 12ln |x|
dy
dx=
sinx cosx tan3 x√x
[cotx− tanx+
3 sec2 x
tanx− 1
2x
]
35. f ′(x) = exe−1 36. ln y = −√10 lnx,
1y
dy
dx= −√10x
,dy
dx= −
√10
x1+√
10
37. (a) logx e =ln elnx
=1
lnx,d
dx[logx e] = −
1x(lnx)2
(b) logx 2 =ln 2lnx
,d
dx[logx 2] = −
ln 2x(lnx)2
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Exercise Set 4.2 135
38. (a) From loga b =ln bln a
for a, b > 0 it follows that log(1/x) e =ln e
ln(1/x)= − 1
lnx, hence
d
dx
[log(1/x) e
]=
1x(lnx)2
(b) log(ln x) e =ln e
ln(lnx)=
1ln(lnx)
, sod
dxlog(ln x) e = −
1(ln(lnx))2
1x lnx
= − 1x(lnx)(ln(lnx))2
39. f(x0) = f(e−1) = −1, f ′(x) = 1x, f ′(x0) = e, y − (−1) = e(x− 1/e) = ex− 1, y = ex− 2
40. y0 = log 10 = 1, y = log x = (log e) lnx,dy
dx
∣∣∣∣x=10
= log e110,
y − 1 =log e10
(x− 10), y =log e10
x+ 1− log e
41. f(x0) = f(−e) = 1, f ′(x)∣∣∣∣x=−e
= −1e,
y − 1 = −1e(x+ e), y = −1
ex
42. y − ln 2 = −12(x+ 2), y = −1
2x+ ln 2− 1
43. Let the equation of the tangent line be y = mx and suppose that it meets the curve at (x0, y0).
Then m =1x
∣∣∣∣x=x0
=1x0
and y0 = mx0 = lnx0. So m =1x0
=lnx0
x0and lnx0 = 1, x0 = e,m =
1e
and the equation of the tangent line is y =1ex.
44. Let y = mx + b be a line tangent to the curve at (x0, y0). Then b is the y-intercept and the
slope of the tangent line is m =1x0
. Moreover, at the point of tangency, mx0 + b = lnx0 or
1x0
x0 + b = lnx0, b = lnx0 − 1, as required.
45. The area of the triangle PQR, given by |PQ||QR|/2 isrequired. |PQ| = w, and, by Exercise 44, |QR| = 1, soarea = w/2.
2
–2
1
x
y
P (w, ln w)Q
R
w
46. Since y = 2 lnx, let y = 2z; then z = lnx and we apply the result of Exercise 45 to find that thearea is, in the x-z plane, w/2. In the x-y plane, since y = 2z, the vertical dimension gets doubled,so the area is w.
47. If x = 0 then y = ln e = 1, anddy
dx=
1x+ e
. But ey = x+ e, sody
dx=
1ey
= e−y.
48. When x = 0, y = − ln(e2) = −2. Next,dy
dx=
1e2 − x
. But ey = e− ln(e2−x) = (e2 − x)−1, so
dy
dx= ey.
January 27, 2005 11:44 L24-ch04 Sheet number 10 Page number 136 black
136 Chapter 4
49. Let y = ln(x+a). Following Exercise 47 we getdy
dx=
1x+ a
= e−y, and when x = 0, y = ln(a) = 0
if a = 1, so let a = 1, then y = ln(x+ 1).
50. Let y = − ln(a− x), thendy
dx=
1a− x
. But ey =1
a− x, so
dy
dx= ey.
If x = 0 then y = − ln(a) = − ln 2 provided a = 2, so y = − ln(2− x).
51. (a) f(x) = lnx; f ′(e2) = lim∆x→0
ln(e2 +∆x)− 2∆x
=d
dx(lnx)
∣∣∣∣x=e2
=1x
∣∣∣∣x=e2
= e−2
(b) f(w) = lnw; f ′(1) = limh→0
ln(1 + h)− ln 1h
= limh→0
ln(1 + h)h
=1w
∣∣∣∣w=1
= 1
52. (a) Let f(x) = ln(cosx), then f(0) = ln(cos 0) = ln 1 = 0, so f ′(0) = limx→0
f(x)− f(0)x
=
limx→0
ln(cosx)x
, and f ′(0) = − tan 0 = 0.
(b) Let f(x) = x√
2, then f(1) = 1, so f ′(1) = limh→0
f(1 + h)− f(1)h
= limh→0
(1 + h)√
2 − 1h
, and
f ′(x) =√2x√
2−1, f ′(1) =√2.
53.d
dx[logb x] = lim
h→0
logb(x+ h)− logb(x)h
= limh→0
1hlogb
(x+ h
x
)Theorem 1.6.2(b)
= limh→0
1hlogb
(1 +
h
x
)
= limv→0
1vx
logb(1 + v) Let v = h/x and note that v → 0 as h→ 0
=1xlimv→0
1vlogb(1 + v) h and v are variable, whereas x is constant
=1xlimv→0
logb(1 + v)1/v Theorem 1.6.2.(c)
=1xlogb lim
v→0(1 + v)1/v Theorem 2.5.5
=1xlogb e Formula 7 of Section 7.1
EXERCISE SET 4.3
1. (a) f ′(x) = 5x4 + 3x2 + 1 ≥ 1 so f is one-to-one on −∞ < x < +∞.
(b) f(1) = 3 so 1 = f−1(3);d
dxf−1(x) =
1f ′(f−1(x))
, (f−1)′(3) =1
f ′(1)=
19
2. (a) f ′(x) = 3x2 + 2ex; for −1 < x < 1, f ′(x) ≥ 2e−1 = 2/e, and for |x| > 1, f ′(x) ≥ 3x2 ≥ 3, sof is increasing and one-to-one
(b) f(0) = 2 so 0 = f−1(2);d
dxf−1(x) =
1f ′(f−1(x))
, (f−1)′(2) =1
f ′(0)=
12
January 27, 2005 11:44 L24-ch04 Sheet number 11 Page number 137 black
Exercise Set 4.3 137
3. f−1(x) =2x− 3, so directly
d
dxf−1(x) = − 2
x2 . Using Formula (1),
f ′(x) =−2
(x+ 3)2, so
1f ′(f−1(x))
= −(1/2)(f−1(x) + 3)2,
d
dxf−1(x) = −(1/2)
(2x
)2
= − 2x2
4. f−1(x) =ex − 1
2, so directly,
d
dxf−1(x) =
ex
2. Next, f ′(x) =
22x+ 1
, and using Formula (1),
d
dxf−1(x) =
2f−1(x) + 12
=ex
2
5. (a) f ′(x) = 2x + 8; f ′ < 0 on (−∞,−4) and f ′ > 0 on (−4,+∞); not enough information. Byinspection, f(1) = 10 = f(−9), so not one-to-one
(b) f ′(x) = 10x4 + 3x2 + 3 ≥ 3 > 0; f ′(x) is positive for all x, so f is one-to-one(c) f ′(x) = 2 + cosx ≥ 1 > 0 for all x, so f is one-to-one(d) f ′(x) = −(ln 2)
( 12
)x< 0 because ln 2 > 0, so f is one-to-one for all x.
6. (a) f ′(x) = 3x2 + 6x = x(3x + 6) changes sign at x = −2, 0, so not enough information; byobservation (of the graph, and using some guesswork), f(−1 +
√3) = −6 = f(−1−
√3), so
f is not one-to-one.
(b) f ′(x) = 5x4 + 24x2 + 2 ≥ 2 > 0; f ′ is positive for all x, so f is one-to-one
(c) f ′(x) =1
(x+ 1)2; f is one-to-one because:
if x1 < x2 < −1 then f ′ > 0 on [x1, x2], so f(x1) = f(x2)if −1 < x1 < x2 then f ′ > 0 on [x1, x2], so f(x1) = f(x2)if x1 < −1 < x2 then f(x1) > 1 > f(x2) since f(x) > 1 on (−∞,−1) and f(x) < 1 on(−1,+∞)
(d) Note that f(x) is only defined for x > 0.d
dxlogb x =
1x ln b
, which is always negative
(0 < b < 1), so f is one-to-one.
7. y = f−1(x), x = f(y) = 5y3 + y − 7,dx
dy= 15y2 + 1,
dy
dx=
115y2 + 1
;
check: 1 = 15y2 dy
dx+
dy
dx,dy
dx=
115y2 + 1
8. y = f−1(x), x = f(y) = 1/y2,dx
dy= −2y−3,
dy
dx= −y3/2;
check: 1 = −2y−3 dy
dx,dy
dx= −y3/2
9. y = f−1(x), x = f(y) = 2y5 + y3 + 1,dx
dy= 10y4 + 3y2,
dy
dx=
110y4 + 3y2 ;
check: 1 = 10y4 dy
dx+ 3y2 dy
dx,dy
dx=
110y4 + 3y2
10. y = f−1(x), x = f(y) = 5y − sin 2y,dx
dy= 5− 2 cos 2y,
dy
dx=
15− 2 cos 2y
;
check: 1 = (5− 2 cos 2y)dy
dx,dy
dx=
15− 2 cos 2y
January 27, 2005 11:44 L24-ch04 Sheet number 12 Page number 138 black
138 Chapter 4
11. 7e7x 12. −10xe−5x2
13. x3ex + 3x2ex = x2ex(x+ 3) 14. − 1x2 e
1/x
15.dy
dx=
(ex + e−x)(ex + e−x)− (ex − e−x)(ex − e−x)(ex + e−x)2
=(e2x + 2 + e−2x)− (e2x − 2 + e−2x)
(ex + e−x)2= 4/(ex + e−x)2
16. ex cos(ex)
17. (x sec2 x+ tanx)ex tan x 18.dy
dx=
(lnx)ex − ex(1/x)(lnx)2
=ex(x lnx− 1)
x(lnx)2
19. (1− 3e3x)e(x−e3x) 20.152x2(1 + 5x3)−1/2 exp(
√1 + 5x3)
21.(x− 1)e−x
1− xe−x=
x− 1ex − x
22.1
cos(ex)[− sin(ex)]ex = −ex tan(ex)
23. f ′(x) = 2x ln 2; y = 2x, ln y = x ln 2,1yy′ = ln 2, y′ = y ln 2 = 2x ln 2
24. f ′(x) = −3−x ln 3; y = 3−x, ln y = −x ln 3, 1yy′ = − ln 3, y′ = −y ln 3 = −3−x ln 3
25. f ′(x) = πsin x(lnπ) cosx;
y = πsin x, ln y = (sinx) lnπ,1yy′ = (lnπ) cosx, y′ = πsin x(lnπ) cosx
26. f ′(x) = πx tan x(lnπ)(x sec2 x+ tanx);
y = πx tan x, ln y = (x tanx) lnπ,1yy′ = (lnπ)(x sec2 x+ tanx)
y′ = πx tan x(lnπ)(x sec2 x+ tanx)
27. ln y = (lnx) ln(x3 − 2x),1y
dy
dx=
3x2 − 2x3 − 2x
lnx+1xln(x3 − 2x),
dy
dx= (x3 − 2x)ln x
[3x2 − 2x3 − 2x
lnx+1xln(x3 − 2x)
]
28. ln y = (sinx) lnx,1y
dy
dx=
sinxx
+ (cosx) lnx,dy
dx= xsin x
[sinxx
+ (cosx) lnx]
29. ln y = (tanx) ln(lnx),1y
dy
dx=
1x lnx
tanx+ (sec2 x) ln(lnx),
dy
dx= (lnx)tan x
[tanxx lnx
+ (sec2 x) ln(lnx)]
January 27, 2005 11:44 L24-ch04 Sheet number 13 Page number 139 black
Exercise Set 4.3 139
30. ln y = (lnx) ln(x2 + 3),1y
dy
dx=
2xx2 + 3
lnx+1xln(x2 + 3),
dy
dx= (x2 + 3)ln x
[2x
x2 + 3lnx+
1xln(x2 + 3)
]
31. f ′(x) = exe−1
32. (a) because xx is not of the form ax where a is constant
(b) y = xx, ln y = x lnx,1yy′ = 1 + lnx, y′ = xx(1 + lnx)
33.3√
1− (3x)2=
3√1− 9x2
34. − 1/2√1−
(x+1
2
)2 = − 1√4− (x+ 1)2
35.1√
1− 1/x2(−1/x2) = − 1
|x|√x2 − 1
36.sinx√
1− cos2 x=
sinx| sinx| =
{1, sinx > 0−1, sinx < 0
37.3x2
1 + (x3)2=
3x2
1 + x6 38.5x4
|x5|√(x5)2 − 1
=5
|x|√x10 − 1
39. y = 1/ tanx = cotx, dy/dx = − csc2 x
40. y = (tan−1 x)−1, dy/dx = −(tan−1 x)−2(
11 + x2
)
41.ex
|x|√x2 − 1
+ ex sec−1 x 42. − 1(cos−1 x)
√1− x2
43. 0 44.3x2(sin−1 x)2√
1− x2+ 2x(sin−1 x)3
45. 0 46. −1/√e2x − 1
47. − 11 + x
(12x−1/2
)= − 1
2(1 + x)√x
48. − 1
2√cot−1 x(1 + x2)
49. (a) Let x = f(y) = cot y, 0 < y < π,−∞ < x < +∞. Then f is differentiable and one-to-oneand f ′(f−1(x)) = − csc2(cot−1 x) = −x2 − 1 = 0, andd
dx[cot−1 x]
∣∣∣∣x=0
= limx→0
1f ′(f−1(x))
= − limx→0
1x2 + 1
= −1.
(b) If x = 0 then, from Exercise 50(a) of Section 1.5,d
dxcot−1 x =
d
dxtan−1 1
x= − 1
x2
11 + (1/x)2
= − 1x2 + 1
. For x = 0, Part (a) shows the same;
thus for −∞ < x < +∞,d
dx[cot−1 x] = − 1
x2 + 1.
(c) For −∞ < u < +∞, by the chain rule it follows thatd
dx[cot−1 u] = − 1
u2 + 1du
dx.
January 27, 2005 11:44 L24-ch04 Sheet number 14 Page number 140 black
140 Chapter 4
50. (a) By the chain rule,d
dx[csc−1 x] =
d
dxsin−1 1
x= − 1
x2
1√1− (1/x)2
=−1
|x|√x2 − 1
(b) By the chain rule,d
dx[csc−1 u] =
du
dx
d
du[csc−1 u] =
−1|u|√u2 − 1
du
dx
51. x3 + x tan−1 y = ey, 3x2 +x
1 + y2 y′ + tan−1 y = eyy′, y′ =
(3x2 + tan−1 y)(1 + y2)(1 + y2)ey − x
52. sin−1(xy) = cos−1(x− y),1√
1− x2y2(xy′ + y) = − 1√
1− (x− y)2(1− y′),
y′ =y√1− (x− y)2 +
√1− x2y2√
1− x2y2 − x√
1− (x− y)2
53. (a) f(x) = x3 − 3x2 + 2x = x(x− 1)(x− 2) so f(0) = f(1) = f(2) = 0 thus f is not one-to-one.
(b) f ′(x) = 3x2 − 6x + 2, f ′(x) = 0 when x =6±√36− 246
= 1 ±√3/3. f ′(x) > 0 (f is
increasing) if x < 1−√3/3, f ′(x) < 0 (f is decreasing) if 1−
√3/3 < x < 1 +
√3/3, so f(x)
takes on values less than f(1−√3/3) on both sides of 1−
√3/3 thus 1−
√3/3 is the largest
value of k.
54. (a) f(x) = x3(x− 2) so f(0) = f(2) = 0 thus f is not one to one.(b) f ′(x) = 4x3− 6x2 = 4x2(x− 3/2), f ′(x) = 0 when x = 0 or 3/2; f is decreasing on (−∞, 3/2]
and increasing on [3/2,+∞) so 3/2 is the smallest value of k.
55. (a) f ′(x) = 4x3 + 3x2 = (4x+ 3)x2 = 0 only at x = 0. But on [0, 2], f ′ has no sign change, so fis one-to-one.
(b) F ′(x) = 2f ′(2g(x))g′(x) so F ′(3) = 2f ′(2g(3))g′(3). By inspection f(1) = 3, sog(3) = f−1(3) = 1 and g′(3) = (f−1)′(3) = 1/f ′(f−1(3)) = 1/f ′(1) = 1/7 becausef ′(x) = 4x3 + 3x2. Thus F ′(3) = 2f ′(2)(1/7) = 2(44)(1/7) = 88/7.F (3) = f(2g(3)) = f(2·1) = f(2) = 24, so the line tangent to F (x) at (3, 25) has the equationy − 25 = (88/7)(x− 3), y = (88/7)x− 89/7.
56. (a) f ′(x) = −e4−x2(2 +
1x2
)< 0 for all x > 0, so f is one-to-one.
(b) By inspection, f(2) = 1/2, so 2 = f−1(1/2) = g(1/2). By inspection,
f ′(2) = −(2 +
14
)= −9
4, and
F ′(1/2) = f ′([g(x)]2)d
dx[g(x)2]
∣∣∣∣x=1/2
= f ′([g(x)]2)2g(x)g′(x)∣∣∣∣x=1/2
= f ′(22)2 · 2 1f ′(g(x))
∣∣∣∣x=1/2
= 4f ′(4)f ′(2)
= 4e−12(2 + 1
16 )(2 + 1
4 )=
339e12 =
113e12
57. (a) f ′(x) = kekx, f ′′(x) = k2ekx, f ′′′(x) = k3ekx, . . . , f (n)(x) = knekx
(b) g′(x) = −ke−kx, g′′(x) = k2e−kx, g′′′(x) = −k3e−kx, . . . , g(n)(x) = (−1)nkne−kx
58.dy
dt= e−λt(ωA cosωt− ωB sinωt) + (−λ)e−λt(A sinωt+B cosωt)
= e−λt[(ωA− λB) cosωt− (ωB + λA) sinωt]
January 27, 2005 11:44 L24-ch04 Sheet number 15 Page number 141 black
Exercise Set 4.3 141
59. f ′(x)=1√2πσ
exp
[−12
(x− µ
σ
)2]
d
dx
[−12
(x− µ
σ
)2]
=1√2πσ
exp
[−12
(x− µ
σ
)2] [−(x− µ
σ
)(1σ
)]
= − 1√2πσ3
(x− µ) exp
[−12
(x− µ
σ
)2]
60. y = Aekt, dy/dt = kAekt = k(Aekt) = ky
61. y = Ae2x +Be−4x, y′ = 2Ae2x − 4Be−4x, y′′ = 4Ae2x + 16Be−4x soy′′ + 2y′ − 8y = (4Ae2x + 16Be−4x) + 2(2Ae2x − 4Be−4x)− 8(Ae2x +Be−4x) = 0
62. (a) y′ = −xe−x + e−x = e−x(1− x), xy′ = xe−x(1− x) = y(1− x)
(b) y′ = −x2e−x2/2 + e−x
2/2 = e−x2/2(1− x2), xy′ = xe−x
2/2(1− x2) = y(1− x2)
63.dy
dx= 100(−0.2)e−0.2x = −20y, k = −0.2
64. ln y = (5x+ 1) ln 3− (x/2) ln 4, soy′/y = 5 ln 3− (1/2) ln 4 = 5 ln 3− ln 2, andy′ = (5 ln 3− ln 2)y
65. ln y = ln 60− ln(5 + 7e−t),y′
y=
7e−t
5 + 7e−t=
7e−t + 5− 55 + 7e−t
= 1− 112y, so
dy
dt= r
(1− y
K
)y, with r = 1,K = 12.
66. (a) 12
00 9
(b) P tends to 12 as t gets large; limt→+∞
P (t) = limt→+∞
605 + 7e−t
=60
5 + 7 limt→+∞
e−t=
605
= 12
(c) the rate of population growth tends to zero
3.2
00 9
67. limh→0
10h − 1h
=d
dx10x∣∣∣∣x=0
=d
dxex ln 10
∣∣∣∣x=0
= ln 10
January 27, 2005 11:44 L24-ch04 Sheet number 16 Page number 142 black
142 Chapter 4
68. limh→0
tan−1(1 + h)− π/4h
=d
dxtan−1 x
∣∣∣∣x=1
=1
1 + x2
∣∣∣∣x=1
=12
69. lim∆x→0
9[sin−1(√
32 +∆x)]2 − π2
∆x=
d
dx(3 sin−1 x)2
∣∣∣∣x=√
3/2= 2(3 sin−1 x)
3√1− x2
∣∣∣∣x=√
3/2
= 2(3π
3)
3√1− (3/4)
= 12π
70. lim∆x→0
(2 + ∆x)(2+∆x) − 4∆x
=d
dxxx∣∣∣∣x=2
=d
dxex ln x
∣∣∣∣x=2
= (1 + lnx)ex ln x∣∣∣∣x=2
= (1 + ln 2)22 = 4(1 + ln 2)
71. limw→2
3 sec−1 w − π
w − 2=
d
dx3 sec−1 x
∣∣∣∣x=2
=3
|2|√22 − 1
=√32
72. limw→1
4(tan−1 w)w − π
w − 1=
d
dx4(tan−1 x)x
∣∣∣∣x=1
=d
dx4ex ln tan−1 x
∣∣∣∣x=1
= 4(tan−1 x)x(ln tan−1 x+ x
1/(1 + x2)tan−1 x
) ∣∣∣∣x=1
= π
(ln(π/4) +
124π
)== 2 + π ln(π/4)
EXERCISE SET 4.4
1. (a) limx→2
x2 − 4x2 + 2x− 8
= limx→2
(x− 2)(x+ 2)(x+ 4)(x− 2)
= limx→2
x+ 2x+ 4
=23
(b) limx→+∞
2x− 53x+ 7
=2− lim
x→+∞
5x
3 + limx→+∞
7x
=23
2. (a)sinxtanx
= sinxcosxsinx
= cosx so limx→0
sinxtanx
= limx→0
cosx = 1
(b)x2 − 1x3 − 1
=(x− 1)(x+ 1)
(x− 1)(x2 + x+ 1)=
x+ 1x2 + x+ 1
so limx→1
x2 − 1x3 − 1
=23
3. Tf (x) = −2(x+ 1), Tg(x) = −3(x+ 1),limit = 2/3
4. Tf (x) = −(x− π
2
), Tg(x) = −
(x− π
2
)limit = 1
5. limx→0
ex
cosx= 1 6. lim
x→3
16x− 13
= 1/5
7. limθ→0
sec2 θ
1= 1 8. lim
t→0
tet + et
−et = −1
9. limx→π+
cosx1
= −1 10. limx→0+
cosx2x
= +∞
11. limx→+∞
1/x1
= 0 12. limx→+∞
3e3x
2x= limx→+∞
9e3x
2= +∞
January 27, 2005 11:44 L24-ch04 Sheet number 17 Page number 143 black
Exercise Set 4.4 143
13. limx→0+
− csc2 x
1/x= limx→0+
−xsin2 x
= limx→0+
−12 sinx cosx
= −∞
14. limx→0+
−1/x(−1/x2)e1/x = lim
x→0+
x
e1/x = 0
15. limx→+∞
100x99
ex= limx→+∞
(100)(99)x98
ex= · · · = lim
x→+∞
(100)(99)(98) · · · (1)ex
= 0
16. limx→0+
cosx/ sinxsec2 x/ tanx
= limx→0+
cos2 x = 1 17. limx→0
2/√1− 4x2
1= 2
18. limx→0
1− 11 + x2
3x2 = limx→0
13(1 + x2)
=13
19. limx→+∞
xe−x = limx→+∞
x
ex= limx→+∞
1ex
= 0
20. limx→π
(x− π) tan(x/2) = limx→π
x− π
cot(x/2)= limx→π
1−(1/2) csc2(x/2)
= −2
21. limx→+∞
x sin(π/x) = limx→+∞
sin(π/x)1/x
= limx→+∞
(−π/x2) cos(π/x)−1/x2 = lim
x→+∞π cos(π/x) = π
22. limx→0+
tanx lnx = limx→0+
lnxcotx
= limx→0+
1/x− csc2 x
= limx→0+
− sin2 x
x= limx→0+
−2 sinx cosx1
= 0
23. limx→(π/2)−
sec 3x cos 5x = limx→(π/2)−
cos 5xcos 3x
= limx→(π/2)−
−5 sin 5x−3 sin 3x =
−5(+1)(−3)(−1) = −5
3
24. limx→π
(x− π) cotx = limx→π
x− π
tanx= limx→π
1sec2 x
= 1
25. y = (1− 3/x)x, limx→+∞
ln y = limx→+∞
ln(1− 3/x)1/x
= limx→+∞
−31− 3/x
= −3, limx→+∞
y = e−3
26. y = (1 + 2x)−3/x, limx→0
ln y = limx→0−3 ln(1 + 2x)
x= limx→0− 61 + 2x
= −6, limx→0
y = e−6
27. y = (ex + x)1/x, limx→0
ln y = limx→0
ln(ex + x)x
= limx→0
ex + 1ex + x
= 2, limx→0
y = e2
28. y = (1 + a/x)bx, limx→+∞
ln y = limx→+∞
b ln(1 + a/x)1/x
= limx→+∞
ab
1 + a/x= ab, lim
x→+∞y = eab
29. y = (2− x)tan(πx/2), limx→1
ln y = limx→1
ln(2− x)cot(πx/2)
= limx→1
2 sin2(πx/2)π(2− x)
= 2/π, limx→1
y = e2/π
30. y= [cos(2/x)]x2, limx→+∞
ln y = limx→+∞
ln cos(2/x)1/x2 = lim
x→+∞
(−2/x2)(− tan(2/x))−2/x3
= limx→+∞
− tan(2/x)1/x
= limx→+∞
(2/x2) sec2(2/x)−1/x2 = −2, lim
x→+∞y = e−2
31. limx→0
(1
sinx− 1x
)= limx→0
x− sinxx sinx
= limx→0
1− cosxx cosx+ sinx
= limx→0
sinx2 cosx− x sinx
= 0
January 27, 2005 11:44 L24-ch04 Sheet number 18 Page number 144 black
144 Chapter 4
32. limx→0
1− cos 3xx2 = lim
x→0
3 sin 3x2x
= limx→0
92cos 3x =
92
33. limx→+∞
(x2 + x)− x2√x2 + x+ x
= limx→+∞
x√x2 + x+ x
= limx→+∞
1√1 + 1/x+ 1
= 1/2
34. limx→0
ex − 1− x
xex − x= limx→0
ex − 1xex + ex − 1
= limx→0
ex
xex + 2ex= 1/2
35. limx→+∞
[x− ln(x2 + 1)] = limx→+∞
[ln ex − ln(x2 + 1)] = limx→+∞
lnex
x2 + 1,
limx→+∞
ex
x2 + 1= limx→+∞
ex
2x= limx→+∞
ex
2= +∞ so lim
x→+∞[x− ln(x2 + 1)] = +∞
36. limx→+∞
lnx
1 + x= limx→+∞
ln1
1/x+ 1= ln(1) = 0
38. (a) limx→+∞
lnxxn
= limx→+∞
1/xnxn−1 = lim
x→+∞
1nxn
= 0
(b) limx→+∞
xn
lnx= limx→+∞
nxn−1
1/x= limx→+∞
nxn = +∞
39. (a) L’Hopital’s Rule does not apply to the problem limx→1
3x2 − 2x+ 13x2 − 2x
because it is not a00form.
(b) limx→1
3x2 − 2x+ 13x2 − 2x
= 2
40. L’Hopital’s Rule does not apply to the probleme3x2−12x+12
x4 − 16, which is of the form
e0
0, and from
which it follows that limx→2−
and limx→2+
exist, with values −∞ if x approaches 2 from the left and
+∞ if from the right. The general limit limx→2
does not exist.
41. limx→+∞
1/(x lnx)1/(2√x)
= limx→+∞
2√x lnx
= 0 0.15
0100 10000
42. y = xx, limx→0+
ln y = limx→0+
lnx1/x
= limx→0+
−x = 0, limx→0+
y = 1 1
00 0.5
January 27, 2005 11:44 L24-ch04 Sheet number 19 Page number 145 black
Exercise Set 4.4 145
25
190 0.5
43. y = (sinx)3/ ln x,
limx→0+
ln y = limx→0+
3 ln sinxlnx
= limx→0+
(3 cosx)x
sinx= 3,
limx→0+
y = e3
4.1
3.31.4 1.6
44. limx→π/2−
4 sec2 x
secx tanx= limx→π/2−
4sinx
= 4
0
–16
0 345. lnx− ex = lnx− 1
e−x=
e−x lnx− 1e−x
;
limx→+∞
e−x lnx = limx→+∞
lnxex
= limx→+∞
1/xex
= 0 by L’Hopital’s Rule,
so limx→+∞
[lnx− ex] = limx→+∞
e−x lnx− 1e−x
= −∞
–0.6
–1.2
0 1246. lim
x→+∞[ln ex − ln(1 + 2ex)] = lim
x→+∞ln
ex
1 + 2ex
= limx→+∞
ln1
e−x + 2= ln
12;
horizontal asymptote y = − ln 2
1.02
1100 10000
47. y = (lnx)1/x,
limx→+∞
ln y = limx→+∞
ln(lnx)x
= limx→+∞
1x lnx
= 0;
limx→+∞
y = 1, y = 1 is the horizontal asymptote
January 27, 2005 11:44 L24-ch04 Sheet number 20 Page number 146 black
146 Chapter 4
48. y =(x+ 1x+ 2
)x, limx→+∞
ln y = limx→+∞
lnx+ 1x+ 21/x
= limx→+∞
−x2
(x+ 1)(x+ 2)= −1;
limx→+∞
y = e−1 is the horizontal asymptote
1
00 50
49. (a) 0 (b) +∞ (c) 0 (d) −∞ (e) +∞ (f) −∞
50. (a) Type 00; y = x(ln a)/(1+ln x); limx→0+
ln y = limx→0+
(ln a) lnx1 + lnx
= limx→0+
(ln a)/x1/x
= limx→0+
ln a = ln a,
limx→0+
y = eln a = a
(b) Type ∞0; same calculation as Part (a) with x→ +∞
(c) Type 1∞; y = (x+ 1)(ln a)/x, limx→0
ln y = limx→0
(ln a) ln(x+ 1)x
= limx→0
ln ax+ 1
= ln a,
limx→0
y = eln a = a
51. limx→+∞
1 + 2 cos 2x1
does not exist, nor is it ±∞; limx→+∞
x+ sin 2xx
= limx→+∞
(1 +
sin 2xx
)= 1
52. limx→+∞
2− cosx3 + cosx
does not exist, nor is it ±∞; limx→+∞
2x− sinx3x+ sinx
= limx→+∞
2− (sinx)/x3 + (sinx)/x
=23
53. limx→+∞
(2 + x cos 2x+ sin 2x) does not exist, nor is it ±∞; limx→+∞
x(2 + sin 2x)x+ 1
= limx→+∞
2 + sin 2x1 + 1/x
,
which does not exist because sin 2x oscillates between −1 and 1 as x→ +∞
54. limx→+∞
(1x+
12cosx+
sinx2x
)does not exist, nor is it ±∞;
limx→+∞
x(2 + sinx)x2 + 1
= limx→+∞
2 + sinxx+ 1/x
= 0
55. limR→0+
V tL e−Rt/L
1=
V t
L
56. (a) limx→π/2
(π/2− x) tanx = limx→π/2
π/2− x
cotx= limx→π/2
−1− csc2 x
= limx→π/2
sin2 x = 1
(b) limx→π/2
(1
π/2− x− tanx
)= limx→π/2
(1
π/2− x− sinx
cosx
)= limx→π/2
cosx− (π/2− x) sinx(π/2− x) cosx
= limx→π/2
−(π/2− x) cosx−(π/2− x) sinx− cosx
= limx→π/2
(π/2− x) sinx+ cosx−(π/2− x) cosx+ 2 sinx
= 0
(c) 1/(π/2− 1.57) ≈ 1255.765534, tan 1.57 ≈ 1255.765592;1/(π/2− 1.57)− tan 1.57 ≈ 0.000058
January 27, 2005 11:44 L24-ch04 Sheet number 21 Page number 147 black
Review Exercises, Chapter 4 147
57. (b) limx→+∞
x(k1/x − 1) = limt→0+
kt − 1t
= limt→0+
(ln k)kt
1= ln k
(c) ln 0.3 = −1.20397, 1024(
1024√0.3− 1
)= −1.20327;
ln 2 = 0.69315, 1024(
1024√2− 1
)= 0.69338
58. If k = −1 then limx→0
(k + cos �x) = k + 1 = 0, so limx→0
k + cos �xx2 = ±∞. Hence k = −1, and by the
rule limx→0
−1 + cos �xx2 = lim
x→0
−� sin �x2x
= limx→0
−�2 cos �x2
= −�2
2= −4 if � = ±2
√2.
59. (a) No; sin(1/x) oscillates as x→ 0. (b) 0.05
–0.05
–0.35 0.35
(c) For the limit as x→ 0+ use the Squeezing Theorem together with the inequalities−x2 ≤ x2 sin(1/x) ≤ x2. For x→ 0− do the same; thus lim
x→0f(x) = 0.
60. (a) Apply the rule to get limx→0
− cos(1/x) + 2x sin(1/x)cosx
which does not exist (nor is it ±∞).
(b) Rewrite as limx→0
[ x
sinx
][x sin(1/x)], but lim
x→0
x
sinx= lim
x→0
1cosx
= 1 and limx→0
x sin(1/x) = 0,
thus limx→0
[ x
sinx
][x sin(1/x)] = (1)(0) = 0
61. limx→0+
sin(1/x)(sinx)/x
, limx→0+
sinxx
= 1 but limx→0+
sin(1/x) does not exist because sin(1/x) oscillates between
−1 and 1 as x→ +∞, so limx→0+
x sin(1/x)sinx
does not exist.
62. Since f(0) = g(0) = 0, then for x = a,f(x)g(x)
=(f(x)− f(0)/(x− a)(g(x)− g(0))/(x− a)
. Now take the limit:
limx→a
f(x)g(x)
= limx→a
(f(x)− f(0)/(x− a)(g(x)− g(0))/(x− a)
=f ′(a)g′(a)
REVIEW EXERCISES, CHAPTER 4
1.1
4(6x− 5)3/4(6) =
32(6x− 5)3/4
2.1
3(x2 + x)2/3(2x+ 1) =
2x+ 13(x2 + x)2/3
3. dy/dx =32
[x− 1x+ 2
]1/2d
dx
[x− 1x+ 2
]=
92(x+ 2)2
[x− 1x+ 2
]1/2
4. dy/dx =x2 4
3(3− 2x)1/3(−2)− (3− 2x)4/3(2x)
x4 =2(3− 2x)1/3(2x− 9)
3x3
January 27, 2005 11:44 L24-ch04 Sheet number 22 Page number 148 black
148 Chapter 4
5. (a) 3x2 + xdy
dx+ y − 2 = 0,
dy
dx=
2− y − 3x2
x
(b) y = (1 + 2x− x3)/x = 1/x+ 2− x2, dy/dx = −1/x2 − 2x
(c)dy
dx=
2− (1/x+ 2− x2)− 3x2
x= −1/x2 − 2x
6. (a) xy = x− y, xdy
dx+ y = 1− dy
dx,dy
dx=
1− y
x+ 1
(b) y(x+ 1) = x, y =x
x+ 1, y′ =
1(x+ 1)2
(c)dy
dx=
1− y
x+ 1=
1− xx+1
1 + x=
1x2 + 1
7. − 1y2
dy
dx− 1x2 = 0 so
dy
dx= −y
2
x2
8. 3x2 − 3y2 dy
dx= 6(x
dy
dx+ y), −(3y2 + 6x)
dy
dx= 6y − 3x2 so
dy
dx=
x2 − 2yy2 + 2x
9.(xdy
dx+ y
)sec(xy) tan(xy) =
dy
dx,dy
dx=
y sec(xy) tan(xy)1− x sec(xy) tan(xy)
10. 2x =(1 + csc y)(− csc2 y)(dy/dx)− (cot y)(− csc y cot y)(dy/dx)
(1 + csc y)2,
2x(1 + csc y)2 = − csc y(csc y + csc2 y − cot2 y)dy
dx,
but csc2 y − cot2 y = 1, sody
dx= −2x(1 + csc y)
csc y
11.dy
dx=
3x4y
,d2y
dx2 =(4y)(3)− (3x)(4dy/dx)
16y2 =12y − 12x(3x/(4y))
16y2 =12y2 − 9x2
16y3 =−3(3x2 − 4y2)
16y3 ,
but 3x2 − 4y2 = 7 sod2y
dx2 =−3(7)16y3 = − 21
16y3
12.dy
dx=
y
y − x,
d2y
dx2 =(y − x)(dy/dx)− y(dy/dx− 1)
(y − x)2=
(y − x)(
y
y − x
)− y
(y
y − x− 1)
(y − x)2
=y2 − 2xy(y − x)3
but y2 − 2xy = −3, sod2y
dx2 = − 3(y − x)3
13.dy
dx= tan(πy/2) + x(π/2)
dy
dxsec2(πy/2),
dy
dx= 1 + (π/4)
dy
dx(2),
dy
dx=
2π − 2
14. Let P (x0, y0) be the required point. The slope of the line 4x − 3y + 1 = 0 is 4/3 so the slope ofthe tangent to y2 = 2x3 at P must be −3/4. By implicit differentiation dy/dx = 3x2/y, so at P ,3x2
0/y0 = −3/4, or y0 = −4x20. But y2
0 = 2x30 because P is on the curve y2 = 2x3. Elimination of
y0 gives 16x40 = 2x3
0, x30(8x0 − 1) = 0, so x0 = 0 or 1/8. From y0 = −4x2
0 it follows that y0 = 0when x0 = 0, and y0 = −1/16 when x0 = 1/8. It does not follow, however, that (0, 0) is a solutionbecause dy/dx = 3x2/y (the slope of the curve as determined by implicit differentiation) is validonly if y = 0. Further analysis shows that the curve is tangent to the x-axis at (0, 0), so the point(1/8,−1/16) is the only solution.
January 27, 2005 11:44 L24-ch04 Sheet number 23 Page number 149 black
Review Exercises, Chapter 4 149
15. Substitute y = mx into x2 +xy+ y2 = 4 to get x2 +mx2 +m2x2 = 4, which has distinct solutionsx = ±2/
√m2 +m+ 1. They are distinct because m2 + m + 1 = (m + 1/2)2 + 3/4 ≥ 3/4, so
m2 +m+ 1 is never zero.Note that the points of intersection occur in pairs (x0, y0) and (−x0, y0). By implicit differentiation,the slope of the tangent line to the ellipse is given by dy/dx = −(2x+ y)/(x+2y). Since the slopeis unchanged if we replace (x, y) with (−x,−y), it follows that the slopes are equal at the two pointof intersection.Finally we must examine the special case x = 0 which cannot be written in the form y = mx. Ifx = 0 then y = ±2, and the formula for dy/dx gives dy/dx = −1/2, so the slopes are equal.
16. Use implicit differentiation to get dy/dx = (y−3x2)/(3y2−x), so dy/dx = 0 if y = 3x2. Substitutethis into x3 − xy + y3 = 0 to obtain 27x6 − 2x3 = 0, x3 = 2/27, x = 3
√2/3 and hence y = 3
√4/3.
17. By implicit differentiation, 3x2 − y− xy′ + 3y2y′ = 0, so y′ = (3x2 − y)/(x− 3y2). This derivativeexists except when x = 3y2. Substituting this into the original equation x3 − xy+ y3 = 0, one has27y6 − 3y3 + y3 = 0, y3(27y3 − 2) = 0. The unique solution in the first quadrant isy = 21/3/3, x = 3y2 = 22/3/3
18. By implicit differentiation, dy/dx = k/(2y) so the slope of the tangent to y2 = kx at (x0, y0) is
k/(2y0) if y0 = 0. The tangent line in this case is y− y0 =k
2y0(x− x0), or 2y0y− 2y2
0 = kx− kx0.
But y20 = kx0 because (x0, y0) is on the curve y2 = kx, so the equation of the tangent line becomes
2y0y − 2kx0 = kx − kx0 which gives y0y = k(x + x0)/2. If y0 = 0, then x0 = 0; the graph ofy2 = kx has a vertical tangent at (0, 0) so its equation is x = 0, but y0y = k(x + x0)/2 gives thesame result when x0 = y0 = 0.
19. y = ln(x+ 1) + 2 ln(x+ 2)− 3 ln(x+ 3)− 4 ln(x+ 4), dy/dx =1
x+ 1+
2x+ 2
− 3x+ 3
− 4x+ 4
20. y =12lnx+
13ln(x+ 1)− ln sinx+ ln cosx, so
dy
dx=
12x
+1
3(x+ 1)− cosx
sinx− sinx
cosx=
5x+ 36x(x+ 1)
− cotx− tanx
21.12x
(2) = 1/x 22. 2(lnx)(1x
)=
2 lnxx
23.1
3x(lnx+ 1)2/324. y = 1
3 ln(x+ 1), y′ =1
3(x+ 1)
25. log10 lnx =ln lnxln 10
, y′ =1
(ln 10)(x lnx)
26. y =1 + lnx/ ln 101− lnx/ ln 10
=ln 10 + lnxln 10− lnx
, y′ =(ln 10− lnx)/x+ (ln 10 + lnx)/x
(ln 10− lnx)2=
2 ln 10x(ln 10− lnx)2
27. y =32lnx+
12ln(1 + x4), y′ =
32x
+2x3
(1 + x4)
28. y =12lnx+ ln cosx− ln(1 + x2), y′ =
12x− sinx
cosx− 2x
1 + x2 =1− 3x2
2x(1 + x2)− tanx
29. y = x2 + 1 so y′ = 2x.
January 27, 2005 11:44 L24-ch04 Sheet number 24 Page number 150 black
150 Chapter 4
30. y = ln(1 + ex + e2x)
(1− ex)(1 + ex + e2x)= − ln(1− ex),
dy
dx=
ex
1− ex
31. y′ = 2e√x + 2xe
√x d
dx
√x = 2e
√x +√xe√x
32. y′ =abe−x
(1 + be−x)233. y′ =
2π(1 + 4x2)
34. y = e(sin−1 x) ln 2, y′ =ln 2√1− x2
2sin−1 x
35. ln y = ex lnx,y′
y= ex
(1x+ lnx
),dy
dx= xe
x
ex(1x+ lnx
)= ex
[xe
x−1 + xex
lnx]
36. ln y =ln(1 + x)
x,y′
y=
x/(1 + x)− ln(1 + x)x2 =
1x(1 + x)
− ln(1 + x)x2 ,
dy
dx=
1x(1 + x)(1/x)−1 − (1 + x)(1/x)
x2 ln(1 + x)
37. y′ =2
|2x+ 1|√(2x+ 1)2 − 1
38. y′ =1
2√cos−1 x2
d
dxcos−1 x2 = − 1√
cos−1 x2
x√1− x4
39. ln y = 3 lnx− 12ln(x2 + 1), y′/y =
3x− x
x2 + 1, y =
3x2√x2 + 1
− x4
(x2 + 1)3/2
40. ln y =13(ln(x2−1)−ln(x2+1)),
y′
y=
13
(2x
x2 − 1− 2xx2 + 1
)=
4x3(x4 − 1)
so y′ =4x
3(x4 − 1)3
√x2 − 1x2 + 1
41. (b) y
x
2
4
6
1 2 3 4
(c)dy
dx=
12− 1x
sody
dx< 0 at x = 1 and
dy
dx> 0 at x = e
(d) The slope is a continuous function which goes from a negative value at x = 1 to a positivevalue at x = e; therefore it must take the value zero between, by the Intermediate ValueTheorem.
(e)dy
dx= 0 when x = 2
42. β = 10 log I − 10 log I0,dβ
dI=
10I ln 10
(a)dβ
dI
]I=10I0
=1
I0 ln 10db/W/m2 (b)
dβ
dI
]I=100I0
=1
10I0 ln 10db/W/m2
(c)dβ
dI
]I=100I0
=1
100I0 ln 10db/W/m2
43. Solvedy
dt= 3
dx
dtgiven y = x lnx. Then
dy
dt=
dy
dx
dx
dt= (1 + lnx)
dx
dt, so 1 + lnx = 3, lnx = 2,
x = e2.
January 27, 2005 11:44 L24-ch04 Sheet number 25 Page number 151 black
Review Exercises, Chapter 4 151
44. x = 2, y = 0; y′ = −2x/(5− x2) = −4 at x = 2, so y − 0 = −4(x− 2) or y = −4x+ 8
y
x
2
2
45. Set y = logb x and solve y′ = 1: y′ =1
x ln b= 1 so
x =1ln b
. The curves intersect when (x, x) lies on the
graph of y = logb x, so x = logb x. From Formula (8),
Section 1.6, logb x =lnxln b
from which lnx = 1, x = e,
ln b = 1/e, b = e1/e ≈ 1.4447.
46. (a) Find the point of intersection: f(x) =√x+ k = lnx. The
slopes are equal, so m1 =1x= m2 =
12√x,√x = 2, x = 4.
Then ln 4 =√4 + k, k = ln 4− 2.
y
x
2
2
(b) Since the slopes are equal m1 =k
2√x
= m2 =1x, so
k√x = 2. At the point of intersection k
√x = lnx, 2 = lnx,
x = e2, k = 2/e.
y
x
0
2
5
47. Where f is differentiable and f ′ = 0, g must be differentiable; this can be inferred from the graphs.In general, however, g need not be differentiable: consider f(x) = x3, g(x) = x1/3.
48. (a) f ′(x) = −3/(x+ 1)2. If x = f(y) = 3/(y + 1) then y = f−1(x) = (3/x)− 1, so
d
dxf−1(x) = − 3
x2 ; and1
f ′(f−1(x))= − (f−1(x) + 1)2
3= − (3/x)2
3= − 3
x2 .
(b) f(x) = ex/2, f ′(x) = 12ex/2. If x = f(y) = ey/2 then y = f−1(x) = 2 lnx, so
d
dxf−1(x) =
2x;
and1
f ′(f−1(x))= 2e−f
−1(x)/2 = 2e− ln x = 2x−1 =2x
49. Let P (x0, y0) be a point on y = e3x then y0 = e3x0 . dy/dx = 3e3x so mtan = 3e3x0 at P and anequation of the tangent line at P is y − y0 = 3e3x0(x − x0), y − e3x0 = 3e3x0(x − x0). If the linepasses through the origin then (0, 0) must satisfy the equation so −e3x0 = −3x0e
3x0 which givesx0 = 1/3 and thus y0 = e. The point is (1/3, e).
50. ln y = ln 5000 + 1.07x;dy/dx
y= 1.07, or
dy
dx= 1.07y
51. ln y = 2x ln 3 + 7x ln 5;dy/dx
y= 2 ln 3 + 7 ln 5, or
dy
dx= (2 ln 3 + 7 ln 5)y
52.dk
dT= k0 exp
[−q(T − T0)
2T0T
](− q
2T 2
)= − qk0
2T 2 exp[−q(T − T0)
2T0T
]
53. y′= aeax sin bx+ beax cos bx and y′′ = (a2 − b2)eax sin bx+ 2abeax cos bx, so y′′ − 2ay′ + (a2 + b2)y= (a2 − b2)eax sin bx+ 2abeax cos bx− 2a(aeax sin bx+ beax cos bx) + (a2 + b2)eax sin bx = 0.
January 27, 2005 11:44 L24-ch04 Sheet number 26 Page number 152 black
152 Chapter 4
54. sin(tan−1 x) = x/√1 + x2 and cos(tan−1 x) = 1/
√1 + x2, and y′ =
11 + x2 , y
′′ =−2x
(1 + x2)2, hence
y′′ + 2 sin y cos3 y =−2x
(1 + x2)2+ 2
x√1 + x2
1(1 + x2)3/2
= 0.
55. (a) 100
200 8
(b) as t tends to +∞, the population tends to 19
limt→+∞
P (t) = limt→+∞
955− 4e−t/4
=95
5− 4 limt→+∞
e−t/4=
955
= 19
(c) the rate of population growth tends to zero 0
–80
0 8
56. (a) y = (1 + x)π, limh→0
(1 + h)π − 1h
=d
dx(1 + x)π
∣∣∣∣x=0
= π(1 + x)π−1∣∣∣∣x=0
= π
(b) Let y =1− lnxlnx
. Then y(e) = 0, and limx→e
1− lnx(x− e) lnx
=dy
dx
∣∣∣∣x=e
= − 1/x(lnx)2
= −1e
57. In the case +∞ − (−∞) the limit is +∞; in the case −∞ − (+∞) the limit is −∞, becauselarge positive (negative) quantities are added to large positive (negative) quantities. The cases+∞− (+∞) and −∞− (−∞) are indeterminate; large numbers of opposite sign are subtracted,and more information about the sizes is needed.
58. (a) when the limit takes the form 0/0 or ∞/∞(b) Not necessarily; only if lim
x→af(x) = 0. Consider g(x) = x; lim
x→0g(x) = 0. For f(x) choose
cosx, x2, and |x|1/2. Then: limx→0
cosxx
does not exist, limx→0
x2
x= 0, and lim
x→0
|x|1/2x2 = +∞.
59. limx→+∞
(ex − x2) = limx→+∞
x2(ex/x2 − 1), but limx→+∞
ex
x2 = limx→+∞
ex
2x= limx→+∞
ex
2= +∞
so limx→+∞
(ex/x2 − 1) = +∞ and thus limx→+∞
x2(ex/x2 − 1) = +∞
60. limx→1
lnxx4 − 1
= limx→1
1/x4x3 =
14; limx→1
√lnx
x4 − 1=
√limx→1
lnxx4 − 1
=12
61. = limx→0
(x2 + 2x)ex
6 sin 3x cos 3x= limx→0
(x2 + 2x)ex
3 sin 6x= limx→0
(x2 + 4x+ 2)ex
18 cos 6x=
19
62. limx→0
ax ln a = ln a