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Exam (elaborations)

Solutions for Electric Circuits, 11th edition by James W. Nilsson |All Chapters

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Solutions for Electric Circuits, 11th edition by James W. Nilsson |All Chapters

Institution
Electric Circuits, 11th Edition
Module
Electric Circuits, 11th edition











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Institution
Electric Circuits, 11th edition
Module
Electric Circuits, 11th edition

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Uploaded on
May 14, 2025
Number of pages
968
Written in
2024/2025
Type
Exam (elaborations)
Contains
Questions & answers

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M

Solution Manual
PR
ES
SI

Electric Circuits
VE

11th Edition
G
R
AD
ES

, 1
M
Circuit Variables
PR

Assessment Problems
ES

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 .
SI
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:
VE
124,274.24 miles 1100 miles
= .
1s xs
Therefore,
1100
x= = 0.00885 = 8.85 × 10−3 s = 8.85 ms.
124,274.24
G
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:
R
$100 billion = $100 × 109.
AD
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
ES
product of ratios:
$100 × 109 1 year 100
· = = $3.17/ms.
1 year 31.5576 × 10 ms 31.5576
9



1–1

, ES
AD
R
G
VE
SI
ES
PR
M

, 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
M
of current:
∫ t
q(t) = i(x) dx.
0
PR
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
∫ ∞
−5000x 20 −5000x ∞ 20 −∞ 0
qtotal = 20e dx = e = (e —e)
0 −5000 0 −5000
ES
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
SI
using Eq. 1.2:
dq d 1 t 1
i= = − + e−αt
dt α2
dt α α2
VE
d 1 d t −αt d 1 −αt
= − e − e
dt α2 dt α dt α2
1 −αt t 1
= 0− e — α e −αt − −α e−αt
α α α2
G
1 1 −αt
= − +t+ e
α α

= te−αt.
R
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
AD
solving for t:
di d
= (te−αt) = e−αt + t(−α)eαt = (1 − αt)e−αt = 0.
dt dt
Since e−αt never equals 0 for a finite value of t, the expression equals 0 only
when (1 − αt) = 0. Thus, t = 1/α will cause the current to be maximum. For
ES
this value of t, the current is
1 −α/α 1 −1
i= e = e .
α α

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