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

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

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A First Course In Differential Equations With Mod
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A First Course in Differential Equations with Mod
Course
A First Course in Differential Equations with Mod

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Uploaded on
August 2, 2025
Number of pages
513
Written in
2025/2026
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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
** Swift Response
** All Chapters included

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




Solution and Answer Guide
ZILL, DIFFERENTIAL EQUATIONS WITH MODELING APPLICATIONS 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)

2
5. Second order; nonlinear because of (dy/dx) or 1 + (dy/dx) 2
6. Second order; nonlinear because of R2
7. Third order; linear
8. Second order; nonlinear because of ẋ 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 — ue u)(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.
2




1

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


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

15. From y = e 3x cos 2x we obtain yj = 3e3x cos 2x—2e 3x sin 2x and yjj = 5e3x cos 2x—12e 3x 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
j
y = 25(1 + tan2 5x) = 25 + 25 tan2 5x = 25 + y 2 .

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 y j =
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)2 −3/2 (— cos x) we have

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.




2

, Solution and Answer Guide: Zill, DIFFERENTIAL EQUATIONS W ith 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
t
2 1 dX –4 –2 2 4
— = 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 y 1 = 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.




3

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