Updated: 9/14/04
Chapter 21 Electromagnetic Induction and
Faraday's Law; AC Circuits
A. Instruction
to students:
Homework:
1) Read carefully all sections except
21-6, -8, and -15.
Sections 21-5 (Electric generators), -9
(Inductance),
-10 (Energy stored in a magnetic field), and
-11 (LR circuit) are
for conceptual understanding only.
2) Do all Examples in the text except
21-6, -7, -8, -11,and -12.
3) Do all sample multiple choice problems posted.
Following formula and constants from Chapters 21 will be given
during the exams. Practice how to use and apply them.
\Phi = BA
emf
= - N (\Delta \Phi) / (\Delta t)
Vp
Ip = Vs Is
emf
= - M (\Delta I) / (\Delta t)
U = L I^2 / 2
V
= I X_L
V
= I X_C
V = I Z
Z
= sqrt[ R^2 + (X_L - X_C)^2 ]
X_L
= 2 \pi f L
X_C
= 1 / ( 2 \pi f C)
B. Biomedical
(and technological) application
Pacemaker in p639 following Eq. 21-8b. (See also Section
19-8.)
Electric generators, Section 21-5, transformers,
Section 21-7, and
electric resonances used in radio and TV, Section 21-14.
C. Lectures
and study guideline
The main objective
of this section is AC circuits of Section 21- 13 and physics leading to
them:
Faraday's law and Lenz's law of Section
21-2, and
" a changing magnetic flux produces an
electric field " of Section 21-4.
The very basic
concept in these is " induction " such as those in
" induced emf, " and " induced current.
"
If you can understand
how electric generators work (in Section 21-5) and how transformers
work (in Section
21-7), you understand the concept of induction. You should then proceed
to the main objective,
AC circuits.
Familiarize yourself
with the terms, their notations, and their units:
Electromotive Force Emf
(V) in p562
Magnetic flux \Phi (Wb,
Weber) 1 Wb
Note: 1 Wb = 1 T
m^2 = 1 N m / A = 1 J / A
= 1 V s
(Remember 1 T = 1 N / A m, from Chapter 20
1 J = 1 N m, from 100A
= 1 V A s, from "power" in Chapter 18)
Resistance R
(Ohm)
Capacitance C (F)
1
F = 1 Coulomb / V
Inductance L
(H, Henry) 1 H = 1 V s / A = 1 Ohm
s
Inductive reactance, or impedance
X_L (Ohm)
Capacitive reactance, or impedance X_C
(Ohm)
(Total) Impedance
Z
(Ohm)
Electromagnetism
described in the six chapters, Chapters 16 - 21, is actually one subject.
As such, if you
could not understand earlier chapters in these chapters, you would not be
able
to understand
Section 21. If this should be the case, do not hesitate to go back
to the earlier
chapters and
to try to understand the materials in them.
The next chapter,
Chapter 22, will be an application of Chapter 21 (thus of all six chapters,
conceptually)
In the second
exam, all formula that were given in the first exam, together with the
new formua
will be given.