Section 9.2: Linear and Almost Linear Systems 535
3
x
Problem 31
3
x
Problem 32
32. 12
y
x



J
At

2,1 : The Jacobian matrix 12
12



J has characteristic equation 240


and real eigenvalues 12.56
 , 21.56
 with different signs. Hence

2,1 is a sad-
dle point.
33. The characteristic equation of the given linear system is

210

, with character-
istic roots 12
,i

.
(a) So if
0
, then 12
,
are complex conjugates with negative real part, and hence
536 Chapter 9: Nonlinear Systems and Phenomena
34. The characteristic equation of the given linear system is

2
10e
.
(a) If 0
, then 12
,1i

  . Thus the characteristic roots are complex conju-
35. (a) If 0h, then we have the familiar system
x
y
, yx
 with circular trajectories
about the origin, which is therefore a center.
(b) The change to polar coordinates as in Example 5 of Section 9.1 is routine, yielding
36. (a) Again, the change of variables is essentially the same as in Example 5 of Section 9.1.
(b) If 2
a
 then the equation

22
rrar
 integrates to give the equation

22
22
ln
ln
2
ar
r
tC aa
  ,
which (after exponentiating) we readily solve for
Section 9.2: Linear and Almost Linear Systems 537
37. The substitution
y
vx in the homogeneous first-order equation
y
Separating the variables and integrating by partial fractions, we get
2
11 21
11
vdx
dv
vv v v x

 




,
or
x
x
x
x
38. The roots of the characteristic equation 20TD

 are given by
2
12
4
,2
TT D


.
We examine the various possibilities individually.
538 Chapter 9: Nonlinear Systems and Phenomena
If the point

,TD lies on the positive D-axis, so 0T but 0D, then 12
iD

 ,
pure imaginary, so we have a stable center.
SECTION 9.3
ECOLOGICAL MODELS:
PREDATORS AND COMPETITORS
1. 200 4 4
2 150 2
yx
y
x





J
At

0, 0 : The Jacobian matrix 200 0
0 150



J has characteristic equation
5
x
Problem 1a
5
u
Problem 1b
Section 9.3: Ecological Applications: Predators and Competitors 539
2. Upon separation of variables, the equation
y
y
3. The effect of using the insecticide is to replace b by bf and a by af in the preda-
tor-prey equations, while leaving p and q unchanged. Hence the new harmful population
is
x
y
Problems 4–7 deal with the competition system
22
60 4 3 , 42 2 3
x
xx xyy yy xy

 ,
that has Jacobian matrix 60 8 3 3
34243
xy x
y
yx
 




J.
4. At

0, 0 the Jacobian matrix 60 0
042



J has characteristic equation
y
540 Chapter 9: Nonlinear Systems and Phenomena
6. At

15, 0 the Jacobian matrix 60 45
03




J has characteristic equation
7. At

6,12 the Jacobian matrix 24 18
36 24





J has characteristic equation
5
Problem 7a
15
20
(0, 21)
Problem 7b
Problems 8–10 deal with the competition system
22
60 3 4 , 42 3 2
x
xx xyy yy xy

 
8. At

0,14 the Jacobian matrix 40
28 42



J has characteristic equation
Section 9.3: Ecological Applications: Predators and Competitors 541
9. At

20,0 the Jacobian matrix 60 80
02




J has characteristic equation
10. At

12,6 the Jacobian matrix 36 48
12 18





J has characteristic equation
5
Problem 10a
15
20
(0, 14)
Problem 10b
Problems 11–13 deal with the predator-prey system
2
5,2
x
x x xy y y xy

 
x
11. At (0,0) the Jacobian matrix 50
02



J has characteristic equation
542 Chapter 9: Nonlinear Systems and Phenomena
12. At

5, 0 the Jacobian matrix 55
03




J has characteristic equation
13. At

2,3 the Jacobian matrix 22
30




J has characteristic equation
5
Problem 13
Problems 14–17 deal with the predator-prey system
22
2, 4
x
xxxyyyyxy

 
Section 9.3: Ecological Applications: Predators and Competitors 543
15. At

0, 4 the Jacobian matrix 60
44



J has characteristic equation
16. At

2,0 the Jacobian matrix 22
02



J has characteristic equation
 
220

 and real eigenvalues 12
 , 22
with different signs. Hence

2,0 is a saddle point of the linearized system 22uuv
, 2vv
 .
17. At

3,1 the Jacobian matrix 33
11



J has characteristic equation
system 33uuv
5
Problem 17
Problems 18 and 19 deal with the predator-prey system
2, 5
x
xxy y yxy

 
544 Chapter 9: Nonlinear Systems and Phenomena
18. At

0, 0 the Jacobian matrix 20
05



J has characteristic equation
19. At

5, 2 the Jacobian matrix 05
20


J has characteristic equation
5
u
Problem 19
Problems 20–22 deal with the predator-prey system
2
3,5
x
x x xy y y xy

  
20. At (0,0) the Jacobian matrix 30
05


J has characteristic equation
Section 9.3: Ecological Applications: Predators and Competitors 545
21. At (3,0) the Jacobian matrix 33
02



J has characteristic equation
22. At

5, 2 the Jacobian matrix 55
20



J has characteristic equation
5
u
Problem 22
Problems 23–25 deal with the predator-prey system
2
7,5
x
x x xy y y xy

 
23. At (0,0) the Jacobian matrix 70


J has characteristic equation
546 Chapter 9: Nonlinear Systems and Phenomena
24. At (7,0) the Jacobian matrix 77
02




J has characteristic equation
25. At

5, 2 the Jacobian matrix 55
20




J has characteristic equation
5
v
Problem 25
26. 2
3
y
x
y
x





J
At

0, 0 : The Jacobian matrix 20
03



J has characteristic equation 2560


Section 9.3: Ecological Applications: Predators and Competitors 547
5
Problem 26
5
Problem 27
27. 242
3
y
x
yx



J
At

0, 0 : The Jacobian matrix 40
03



J has characteristic equation
27120

 and negative real eigenvalues 14
 , 23
 . Hence

0, 0 is a nod-
al sink.
548 Chapter 9: Nonlinear Systems and Phenomena
28. 2162
4
y
x
y
x




J
At (0,0) : The Jacobian matrix 16 0
04


J has characteristic equation
15
Problem 28
29.
11
23
22
242
x
yx
yx

 




J
Section 9.3: Ecological Applications: Predators and Competitors 549
At

3, 0 : The Jacobian matrix 332
02




J has characteristic equation
2560

 and negative real eigenvalues 13
 , 22
 . Hence

3, 0 is a nodal
sink.
At

2, 2 : The Jacobian matrix 21



J has characteristic equation
5
Problem 29
10
Problem 30
30.
11
23
22
11
1
55
x
yx
yx

 





J
550 Chapter 9: Nonlinear Systems and Phenomena
At

3, 0 : The Jacobian matrix 332
02




J has characteristic equation
217 17 0
55

 and negative real eigenvalues 13
 , 2
17
5
 . Hence

3, 0 is a
nodal sink.
31.
11
23
44
2
x
yx
yx

  



J
At

0, 0 : The Jacobian matrix 30
02



J has characteristic equation 260


and real eigenvalues 12
 , 23
of opposite sign. Hence

0, 0 is a saddle point.
5
(2, 4)
Problem 31
75
100
(30, 60)
Problem 32
32. 630
44660
xy x
yxy





J
At

0, 0 : The Jacobian matrix 30 0
060



J has characteristic equation
290 1800 0

 
and positive real eigenvalues 130
, 260
. Hence

0, 0 is a
nodal source.
At

0, 20 : The Jacobian matrix 50 0


J has characteristic equation
At

30,60 : The Jacobian matrix 90 30
240 180



J has characteristic equation
2240 9000 0

 and negative real eigenvalues 1231.05
 , 238.95
 . Hence

30,60 is a nodal sink.
552 Chapter 9: Nonlinear Systems and Phenomena
33. 630
44660
xy x
yxy





J
At

0, 0 : The Jacobian matrix 30 0
080



J has characteristic equation
2110 2400 0

 and positive real eigenvalues 130
, 280
. Hence

0, 0 is a
nodal source.
At

4, 22 : The Jacobian matrix 84
44 88




J has characteristic equation
296 880 0

 and negative real eigenvalues 185.736
 , 210.264
 . Hence

4, 22 is a nodal sink.
40
Problem 33
20
Problem 34
Section 9.4: Nonlinear Mechanical Systems 553
34. 430
22820
xy x
yxy
 




J
At

0, 0 : The Jacobian matrix 30 0
020



J has characteristic equation
250 600 0

 and positive real eigenvalues 120
, 230
. Hence

0, 0 is a
nodal source.
At

10,10 : The Jacobian matrix 20 10
20 40




J has characteristic equation
260 1000 0

 
and complex conjugate eigenvalues
12
,3010i
  with negative
real part. Hence

10,10 is a spiral sink.
x
SECTION 9.4
NONLINEAR MECHANICAL SYSTEMS
In each of Problems 1–4 we need only substitute the familiar power series for the exponential,
sine, and cosine functions, and then discard all higher-order terms. For each problem we give
the corresponding linear system, the eigenvalues 1
and 2
, and the type of this critical point.
1. 2
1
11 2 2
2
x
xx yxy

   


3
1
44
6
y
xyy xy

   


554 Chapter 9: Nonlinear Systems and Phenomena
0
5
y
Problem 1
2. 33
11
22
66
x
xx yy xy
 

 
 

33
11
22
x
x
y
xx yy xy
 
  
 

3. 2
1
1212
2
x
xx y xy

  


y