Solution Manual For A First Course in Differential Equations with Modeling Applications, 12th Edition Dennis G. Zill

A First Course in Differential
Equations with Modeling
Applications, 12th Edition by
Dennis G. Zill




Complete Chapter Solutions Manual are
included (Ch 1 to 9)




** Immediate Download
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,Solution and Answer Guide: Zill, DIFFERENTIAL EQUATIONS With MODELING APPLICATIONS 2024, 9780357760192; Chapter #1:
Introduction to Differential Equations




Solution and Answer Guide
ZILL, DIFFERENTIALEQUATIONSWITHMODELINGAPPLICATIONS 2024, 9780357760192; CHAPTER
#1: INTRODUCTION TO DIFFERENTIAL EQUATIONS


TABLE OF CONTENTS
End of Section Solutions .................................................................................................................................... 1
Exercises 1.1 ................................................................................................................................................ 1
Exercises 1.2 .............................................................................................................................................. 14
Exercises 1.3 .............................................................................................................................................. 22
Chapter 1 in Review Solutions......................................................................................................................... 30




END OF SECTION SOLUTIONS
EXERCISES 1.1
1. Second order; linear
2. Third order; nonlinear because of (dy/dx)4
3. Fourth order; linear
4. Second order; nonlinear because of cos(r + u)
√
5. Second order; nonlinear because of (dy/dx)2 or 1 + (dy/dx)2
6. Second order; nonlinear because of R2
7. Third order; linear
8. Second order; nonlinear because of x˙ 2
9. First order; nonlinear because of sin (dy/dx)
10. First order; linear
11. Writing the differential equation in the form x(dy/dx) + y2 = 1, we see that it is nonlinear in y because of
y2. However, writing it in the form (y2 — 1)(dx/dy) + x = 0, we see that it is linear in x.
12. Writing the differential equation in the form u(dv/du) + (1 + u)v = ueu we see that it is linear in v.
However, writing it in the form (v + uv — ueu)(du/dv) + u = 0, we see that it is nonlinear in u.
13. From y = e− x/2
we obtain yj = — 1 e− x/2
. Then 2yj + y = —e− x/2
+ e− x/2 = 0.
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,Solution and Answer Guide: Zill, DIFFERENTIAL EQUATIONS With MODELING APPLICATIONS 2024, 9780357760192; Chapter #1:
Introduction to Differential Equations


66
14. From y = — e—20t we obtain dy/dt = 24e−20t , so that
5 5
dy + 20y = 24e−20t 6 6 −20t
+ 20 — e = 24.
dt 5 5

15. From y = e3x cos 2x we obtain yj = 3e3x cos 2x—2e3x sin 2x and yjj = 5e3x cos 2x—12e3x sin 2x, so that yjj
— 6yj + 13y = 0.
j
16. From y = — cos x ln(sec x + tan x) we obtain y = —1 + sin x ln(sec x + tan x) and
jj jj
y = tan x + cos x ln(sec x + tan x). Then y + y = tan x.
17. The domain of the function, found by solving x+2 ≥ 0, is [—2, ∞). From yj = 1+2(x+2)−1/2
we have
j 1/2−
(y —x)y = (y — x)[1 + (2(x + 2) ]

= y — x + 2(y —x)(x + 2)−1/2

= y — x + 2[x + 4(x + 2)1/2 —x](x + 2)−1/2

= y — x + 8(x + 2)1/2(x + 2)−1/2 = y — x + 8.

An interval of definition for the solution of the differential equation is (—2, ∞) because yj is not defined at x
= —2.
18. Since tan x is not defined for x = π/2 + nπ, n an integer, the domain of y = 5 tan 5x is
{x 5x /= π/2 + nπ}
or {x x /= π/10 + nπ/5}. From y j= 25 sec 25x we have

yj = 25(1 + tan2 5x) = 25 + 25 tan2 5x = 25 + y2.

An interval of definition for the solution of the differential equation is (—π/10, π/10). An- other interval is
(π/10, 3π/10), and so on.
19. The domain of the function is {x 4 — x2 /= 0} or {x x /= —2 or x /= 2}. From yj =
2x/(4 — x2)2 we have
1 2
= 2xy2.
yj = 2x
4 —x2
An interval of definition for the solution of the differential equation is (—2, 2). Other inter- vals are (—∞,
—2) and (2, ∞).
√
20. The function is y = 1/ 1 — sin x , whose domain is obtained from 1 — sin x /= 0 or sin x /= 1.
Thus, the domain is {x x /= π/2 + 2nπ}. From y j= — (11 — sin x) −3/2 (— cos x) we have
2

2yj = (1 — sin x)−3/2 cos x = [(1 — sin x)−1/2]3 cos x = y3 cos x.

An interval of definition for the solution of the differential equation is (π/2, 5π/2). Another one is (5π/2,
9π/2), and so on.



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, Solution and Answer Guide: Zill, DIFFERENTIAL EQUATIONS With MODELING APPLICATIONS 2024, 9780357760192; Chapter #1:
Introduction to Differential Equations




21. Writing ln(2X — 1) — ln(X — 1) = t and differentiating x

implicitly we obtain 4


— =1 2
2X — 1 dt X — 1 dt

2 1 dX –4 –2 2 4
t
— =1
2X — 1 X —1 dt
–2


–4
dX
= —(2X — 1)(X — 1) = (X — 1)(1 — 2X).
dt
Exponentiating both sides of the implicit solution we obtain

2X — 1
= et
X—1
2X — 1 = Xet — et

(et — 1) = (et — 2)X
et 1
X= .
et — 2
Solving et — 2 = 0 we get t = ln 2. Thus, the solution is defined on (—∞, ln 2) or on (ln 2, ∞). The graph of
the solution defined on (—∞, ln 2) is dashed, and the graph of the solution defined on (ln 2, ∞) is solid.

22. Implicitly differentiating the solution, we obtain y

2 dy dy 4

—2x — 4xy + 2y =0
dx dx 2
—x2 dy — 2xy dx + y dy = 0
x
2xy dx + (x2 — y)dy = 0. –4 –2 2 4

Using the quadratic formula to solve y2 — 2x2y — 1 = 0 –2
√ √
for y, we get y = 2x2 ± 4x4 + 4 /2 = x2 ± x4 + 1 .
√ –4
Thus, two explicit solutions are y1 = x2 + x4 + 1 and
√
y2 = x2 — x4 + 1 . Both solutions are defined on (—∞, ∞).
The graph of y1(x) is solid and the graph of y2 is dashed.




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