9-6
1. (a) By the model: Let dx
dt = 0 and dy
dt = 0 ⇒ x = 20 , y = 500
x 20 20 30 20 10
y 500 300 500 700 500 dx
dt 0 −0.4 0 0.4 0
dy
dt 0 0 −25 0 25
dy
dx 0 ∞ 0 −∞
figure 1
By the graph , we can know that it start (700,20) with x decreasing , y increases. Up to the level, with x increasing , y decreases. To end up , it get to the equilibrium.
So x is the predator and y is the prey. Moreover, the prey is restricted by the number of the predators. Furthermore, the food about the predators is only y because x decreases with y decreasing .
(b) By the model: Let dx
dt = 0 and dy
dt = 0 ⇒ x = 187.5 , y = 27.08 x 187.5 187.5 87.5 187.5 287.5 y 27.08 17.08 30.42 37.08 23.75 dx
dt 0 11.25 0 −11.25 0
dy
dt 0 0 −0.24 0 0.19
dy
dx 0 −∞ 0 ∞
By the graph , we can know that it start (187.5,17.08) with y increasing , x decreases. Up to the level, with y decreasing , x increases. To end up , it get to the equilibrium.
So y is the predator and x is the prey. Moreover, the prey is restricted by the number of the predators and the resources of environment. Furthermore, the food about the predators is only y because x decreases with y decreasing.
7. By the graphs, the phase trajectory is following as:
10. (a)
dA
dt = A(2 − 0.01L) = 0 dL
dt = L(−0.5 + 0.0001A) = 0
⇒
(2 − 0.01L) = 0 (−0.5 + 0.0001A) = 0
⇒
L = 200 A = 5000
the point (A, L) = (5000, 200) is inside the curve. If the initial value is the point , the phase trajectory is only a point.
(b) dL
dA = −0.5L + 0.0001AL 2A − 0.01AL
(c)(d) The phase trajectory is the following as:
(e) The graph about the aphids and lady-bug populations as functions of t is following as:
Chapter 9 Problem Plus
1. Solve the equation: dy
dx = y(y − 2)(y − 4) ⇒ 1 8( 1
y − 4 +1 y − 2
y − 2)dy = dx ⇒ y = 2 ± 2
√1 − c0e8x
(a) (i) y(0) = −0.3 ⇒ c0 = 0.2439 ⇒ y(x) = 2 − 2
√1 − 0.2439e8x
(ii) y(0) = 1 ⇒ c0 = −3 ⇒ y(x) = 2 − 2
√1 + 3e8x
(iii) y(0) = 3 ⇒ c0 = −3 ⇒ y(x) = 2 + 2
√1 + 3e8x
(iv) y(0) = 4.3 ⇒ c0 = 0.2439 ⇒ y(x) = 2 + 2
√1 + 0.2439e8x
(b) y0 = c ⇒ c0 = 1 − 4
(2 − c)2 ⇒ Since y(x) = 2 ± 2
√1 − c0e8x , when lim
x→∞y(x) is finite
⇒ 1 − 4
(2 − c)2 ≤ 0 ⇒ 0 ≤ c ≤ 4 3.
(a) Up to the graph the question, we sketch y(0)=1 and get the graph as following:
we estimate that when x = 0.3, y = 0.8
(b) h = 0.1, x0 = 0, y0 = 1 and Euler’s method:yn= yn−1+ hyn0
⇒ yn= yn−1+ h(x2n−1− y2n−1)
y1 = 1 + 0.1(02− 12) = 0.9, y2 = 1 + 0.1(0.12− 0.92) = 0.82, y3 = 1 + 0.1(0.2 − 0.822) = 0.7576
(c) The center of the horizontal line segments of the direction field are field are located on the lines y=x and y=-x. When a solution curve crosses one of these lines, it has a local maximum or minimum.
9. dr
dt + 2tr = r ⇒ dr
dt = r(1 − 2t) ⇒ dr
r = (1 − 2t)dt ⇒ ln(r) = t − t2+ c0 ⇒ r(t) = c1et−t2 take r(0) = 5 into the equation ⇒ c1 = 5 ⇒ r(t) = 5 et−t2
12. dy
dx = 3 x2ey ⇒ e−ydy = 3 x2dx ⇒ −e−y = c0+ x3 ⇒ y(x) = − ln(−c0 − x3)
⇒ Take y(0) = 1 into the equation ⇒ c0 = −e−1 ⇒ y(x) = − ln(e−1− x3)
14.
y = ekx Differentiate
==========⇒ dy
dx = kekx eliminate k,let k=ln yx
==============⇒ dy
dx = y ln y Orthogonal x
=========⇒
Trajectories dy
dx = −x y ln y
integrate
=======⇒ 1
2y2ln y −1
4y2 = −1 2 x2+ c
=
=⇒ y2ln y − 1
2y2+ x2 = C
10-1
3.
4.
9.
(a)
(b)
x =√
t V x2 = t . . . (1) , y = 1 − t . . . (2)
(1) + (2) : x2+ y = 1, but x > 0 ⇒ x2+ y = 1 and x > 0
10.
(a)
(b) y = t3 ⇒ t = √3
y, x = t2 ======⇒ x = yt=sqrt[3]y 23
13.
(a)
(b) x = sin t . . . (1), y = csc t . . . (2)
(1)×(2):x × y = 1 by(1) and (2) :x > 0 and y > 0 ⇒ xy = 1 , x > 0, y > 0
16.
(a)
(b) x =√
t + 1 ⇒ x2 = t + 1 . . . (1) y =√
t − 1 ⇒ y2 = t − 1 . . . (2).
(1)−(2):x2− y2 = 2 by (1) and (2): x > 0 and y > 0.
So x2− y2 = 2 where x > 0 and y > 0
21. x = 5 sin t , y = 2 cos t ⇒ sin t = x
5, cos t = y
2 ⇒ sin2t + cos2t = 1 ⇒ (x
5)2+ (y
2)2 = 1.
The motion is from (0, −2) to (0, −2) and moves clockwise around the ellipse ( (x
5)2+ (y
2)2 = 1 ) 3 times. So the matched graph is V.
28. (a) x = t4− t + 1 = (t4+ 1) − t > 0 ∀t ∈ R and y = t2 ≥ 0 ⇒ the graph is in the first quadrant.
(b) x = t2− 2t = t(t − 2) and y =√
t ≥ 0. x is negative and y is positive for 0 ≤ t ≤ 2 So the matched graph is I.
(c) x = sin 2t has period π. y(t + 2π) = sin(t + 2π + sin(2(t + 2π))) = sin(t + sin(2t)) = y(t) has period 2π. These equations match graph II since x cycles through the values -1 to 1 twice as y cycles through those values once.
(d) x = cos 5t has the period 2π
5 and y = sin 2t has the period π. And the graph is through (1, 0) for t = 2kπ and (−1, 0) for t = (2k + 1)π. So the matched graph is VI.
(e) x = t + sin 4t and y = t2+ cos 3t. As t becomes large , t and t2 is dominant term. So the graph looks like the graph of y = x2 with the oscillations. So the matched graph is IV.
(f) x = sin 2t
4 + t2 and y = cos 2t
4 + t2. As t → ∞, x → 0 and y → 0 So the matched graph is III.
10-2
2. x = 1
t ⇒ dx dt = −1
t2 and y =√
te−t ⇒ dy
dt = e−tt−12 (1
2 − t). So dy
dx = e−tt32(t −1 2) 5. x = t cos t ⇒ dx
dt = cos t − t sin t and y = t sin t ⇒ dy
dt = sin t + t cos t. So t = π ,dy
dx = −π
−1 = π Moreover, the tangent line is y − y(π) = π(x − x(π) ⇒ y = πx + π2
6. x = cos θ + sin 2θ ⇒ x(0) = 1 and y = sin θ + cos 2θ ⇒ y(0) = 1.
dx
dθ = − sin θ + 2 cos θ and dy
dt = cos θ − 2 sin 2θ. So t = 0 ,dy dx = 1
2. So the tangent line is y = 1
2x + 1 2. 11. x = t2+ 1 and y = t2+ t ⇒ dx
dt = 2t and dy
dt = 2t + 1. So dy
dx = 2t + 1 2t . Moreover, ddydx
dt = −1 2t2, d2y
dx2 =
ddydx dt dx dt
=
−1 2t2
2t = −1
4t3. So the curve is concave upward as d2y
dx2 > 0 ⇒ t < 0 16. x = cos 2t and y = cos t ⇒ dx
dt = −2 sin 2t and dy
dt = − sin t. So dy
dx = 1
4 cos t = sec t 4 . Moreover, ddydx
dt = sec t tan t 4 , d2y
dx2 =
ddydx dt dx dt
=
sec t tan t 4
−2 sin 2t = − sec3t
16 . So the curve is concave upward as d2y
dx2 > 0 ⇒ π
2 < t < π
30. x = 3t2+ 1 and y = 2t3+ 1 ⇒ dx
dt = 6t and dy
dt = 6t2 ⇒ dy dx = t
The tangent line is y − (2t3+ 1) = t(x − (3t2+ 1)) and passes through x = 4, y = 3.
So 2 − 2t3 = 3t − 3t3 ⇒ t3− 3t + 2 = 0 ⇒ (t + 2)(t − 1)2 = 0 ⇒ t = −2 or t = 1.
The tangent line is y − 3 = x − 4 or y − 3 = −2(x − 4).
31. The area is 4 Z a
0
y dx x=a cos θ,y=b sin θ
===========⇒ 4 Z 0
π 2
b sin θa(− sin θ) dθ = 4ab Z π2
0
sin2θdθ = abπ
41. dx
dt = 6t , dy
dt = 6t2, Arc length=
Z 1 0
p(6t)2 + (6t2)2dt ⇒ 6 Z 1
0
t√
t2+ 1 dt = 2(t2+1)(32)
1 0 = 4√
2−2
44. dx
dt = −3 sin t + 3 sin 3t and dy
dt = 3 cos t − 3 cos 3t, Arc length =
Z π 0
3p
(sin 3t − sin t)2+ (cos 3t − cos t)2dt = Z π
0
3√
2 − 2 sin 3t sin t − 2 cos 3t cos t dt
= Z π
0
3p
2 + cos 4t − cos 2t − (cos 4t + cos 2t) dt = 6 Z π
0
r1 − cos 2t 2
= 6 Z π
sin t dt = −6 cos t
π = 12
62. By the formula:
The area of surface = Z 1
0
2π 3t2p
(3 − 3t2)2 + (6t)2dt = 18π Z 1
0
t2p
(t2− 1)2+ (2t)2dt
= 18π Z 1
0
t2(t2+ 1) dt = 18π(1 5 +1
3) = 48 5 π 63. By the formula:
The area of surface = Z π2
0
2π a sin3θ q
(−3a cos2θ sin θ)2+ (3a cos θ sin2θ)2dθ
= 2πa Z π2
0
sin3θ q
(3a cos θ sin θ)(cos θ2+ sin2θ) dθ
= 6πa2 Z π2
0
sin4θ cos θ dθ = 6 5πa2