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Electric Circuits (11th Edition, James W. Nilsson & Susan Riedel) – Instructor’s Solutions Manual with Detailed Chapter Solutions

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This document contains the complete Instructor’s Solutions Manual for Electric Circuits, 11th Edition by James W. Nilsson and Susan Riedel. It includes fully worked solutions to all end-of-chapter problems, assessment problems, and conceptual questions. Each solution features step-by-step calculations, annotated reasoning, and circuit analyses aligned with the structure of the textbook. This manual is ideal for students seeking detailed guidance, instructors preparing coursework, and anyone needing thorough explanations for circuit theory exercises.

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Institución
Electric Circuits
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Institución
Electric Circuits
Grado
Electric Circuits

Información del documento

Subido en
29 de noviembre de 2025
Número de páginas
1261
Escrito en
2025/2026
Tipo
Examen
Contiene
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INSTRUCTOR'S
SOLUTIONS
MANUAL

, Circuit Variables
1
Assessment Problems

AP 1.1 Use a product of ratios to convert two-thirds the speed of light from meters
per second to miles per second:
✓ ◆
2 3 × 108 m · 100 cm · 1 in · 1 ft · 1 mile = 124,274.24 miles .
3 1s 1m 2.54 cm 12 in 5280 feet 1s
Now set up a proportion to determine how long it takes this signal to travel
1100 miles:
124,274.24 miles 1100 miles
= .
1s xs
Therefore,
1100
x= = 0.00885 = 8.85 × 10—3 s = 8.85 ms.
124,274.24
AP 1.2 To solve this problem we use a product of ratios to change units from
dollars/year to dollars/millisecond. We begin by expressing $10 billion in
scientific notation:

$100 billion = $100 × 109.

Now we determine the number of milliseconds in one year, again using a
product of ratios:
1 year 1 day 1 hour 1 min 1 sec 1 year
· · · · = .
365.25 days 24 hours 60 mins 60 secs 1000 ms 31.5576 × 109 ms
Now we can convert from dollars/year to dollars/millisecond, again with a
product of ratios:
$100 × 109 1 year 100
· = = $3.17/ms.
1 year 31.5576 × 109 ms 31.5576

1–1

, 1–2 CHAPTER 1. Circuit Variables

AP 1.3 Remember from Eq. 1.2, current is the time rate of change of charge, or i = dqdt
In this problem, we are given the current and asked to find the total charge.
To do this, we must integrate Eq. 1.2 to find an expression for charge in terms
of current:
Z t
q(t) = i(x) dx.
0

We are given the expression for current, i, which can be substituted into the
above expression. To find the total charge, we let t → ∞ in the integral. Thus
we have
Z ∞
—5000x 20 —5000x ∞ 20 —∞ 0
qtotal = 20e dx = e = (e —e)
0 —5000 0 —5000
20 20
= (0 — 1) = = 0.004 C = 4000 µC.
—5000 5000
AP 1.4 Recall from Eq. 1.2 that current is the time rate of change of charge, or
i = dqdt. In this problem we are given an expression for the charge, and asked to
find the maximum current. First we will find an expression for the current
using Eq. 1.2:

dq td 1 ◆ —↵t
1
i= = — + e
dt dt ↵2 ↵ ↵2
✓ ◆ ✓ ◆ ✓ ◆
d 1 d t —↵t d 1 —↵t
= — e — e
dt ↵2 dt ↵ dt ↵2
✓ ◆ ✓ ◆
1 —↵t — ↵t e—↵t 1
=0— e — —↵ e—↵t
↵ ↵ ↵2
✓ ◆
1 1
= — +t+ e—↵t
↵ ↵

= te—↵t.

Now that we have an expression for the current, we can find the maximum
value of the current by setting the first derivative of the current to zero and
solving for t:
di d
= (te—↵t) = e—↵t + t(—↵)e↵t = (1 — ↵t)e—↵t = 0.
dt dt
Since e—↵t never equals 0 for a finite value of t, the expression equals 0 only
when (1 — ↵t) = 0. Thus, t = 1/↵ will cause the current to be maximum. For
this value of t, the current is
1 —↵/↵ 1 —1
i= e = e .
↵ ↵



© 2019 Pearson Education, Inc., 330 Hudson Street, NY, NY 10013. All rights reserved. This material is protected under all copyright laws as they currently exist.
No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.

, Problems 1–3

Remember in the problem statement, ↵ = 0.03679. Using this value for ↵,
1
i= e—1 ~
= 10 A.
0.03679
AP 1.5 Start by drawing a picture of the circuit described in the problem statement:




Also sketch the four figures from Fig. 1.6:




[a] Now we have to match the voltage and current shown in the first figure
with the polarities shown in Fig. 1.6. Remember that 4A of current
entering Terminal 2 is the same as 4A of current leaving Terminal 1. We
get
(a) v = —20 V, i = —4 A; (b) v = —20 V, i = 4 A;
(c) v = 20 V, i = —4 A; (d) v = 20 V, i = 4 A.
[b] Using the reference system in Fig. 1.6(a) and the passive sign convention,
p = vi = (—20)(—4) = 80 W.
[c] Since the power is greater than 0, the box is absorbing power.

AP 1.6 [a] Applying the passive sign convention to the power equation using the
voltage and current polarities shown in Fig. 1.5, p = vi. To find the time
at which the power is maximum, find the first derivative of the power
with respect to time, set the resulting expression equal to zero, and solve
for time:
p = (80,000te—500t)(15te—500t) = 120 × 104t2e—1000t;
dp
= 240 × 104te—1000t — 120 × 107t2e—1000t = 0.
dt
Therefore,
240 × 104 — 120 × 107t = 0.



© 2019 Pearson Education, Inc., 330 Hudson Street, NY, NY 10013. All rights reserved. This material is protected under all copyright laws as they currently exist.
No portion of this material may be reproduced, in any form or by any means, without permission in writing from the publisher.
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