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Induction and Alternating Current with teacher's notes

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Section 22-1<br />

Teaching Tip<br />

Remind students that, as discussed<br />

in Chapter 21, electric<br />

charges that move through a<br />

magnetic field experience a magnetic<br />

force. The magnitude of this<br />

force is qvB. When charges are at<br />

rest <strong>with</strong> respect to the magnetic<br />

field (v = 0 m/s), they do not<br />

experience a magnetic force.<br />

Visual Strategy<br />

Figure 22-1<br />

Be sure students underst<strong>and</strong> the<br />

conditions required to induce a<br />

current in a circuit.<br />

Why is a current generated in<br />

Q a moving conductor in a<br />

magnetic field but not in a moving<br />

insulator in the same magnetic<br />

field?<br />

Charges experience a force in<br />

A both cases. In conductors, the<br />

electrons are free to move under<br />

the influence of the magnetic<br />

force. Electrons in an insulator<br />

feel the same force but are not<br />

free to move.<br />

Q<br />

What is the condition<br />

required for current to exist in<br />

the circuit shown in this figure?<br />

There must be relative<br />

A motion between the circuit<br />

<strong>and</strong> the magnetic field; when the<br />

two are at rest relative to one<br />

another, charges do not experience<br />

a magnetic force, so they<br />

remain at rest.<br />

794<br />

22-1 SECTION OBJECTIVES<br />

• Describe how the change in<br />

the number of magnetic field<br />

lines through a circuit loop<br />

affects the magnitude <strong>and</strong><br />

direction of the induced<br />

current.<br />

• Apply Lenz’s law to<br />

determine the direction of an<br />

induced current.<br />

• Calculate the induced emf<br />

<strong>and</strong> current using Faraday’s<br />

law of induction.<br />

electromagnetic induction<br />

the production of an emf in a<br />

conducting circuit by a change in<br />

the strength, position, or orientation<br />

of an external magnetic field<br />

Figure 22-1<br />

When the circuit loop<br />

crosses the lines of the<br />

magnetic field, a current<br />

is induced in the circuit,<br />

as indicated by the<br />

movement of the<br />

galvanometer needle.<br />

794<br />

Chapter 22<br />

100<br />

200<br />

300<br />

400<br />

500<br />

600<br />

700<br />

800<br />

900<br />

0 <br />

22-1<br />

Induced current<br />

MAGNETIC FIELDS AND INDUCED EMFS<br />

Recall that in Chapter 20 you were asked if it was possible to produce an electric<br />

current using only wires <strong>and</strong> no battery. So far, all electric circuits that you<br />

have studied have used a battery or an electrical power supply to create a<br />

potential difference <strong>with</strong>in a circuit. In both of these cases, an emf increases<br />

the electrical potential energy of charges in the circuit, causing them to move<br />

through the circuit <strong>and</strong> create a current.<br />

It is also possible to induce a current in a circuit <strong>with</strong>out the use of a battery<br />

or an electrical power supply. Just as a magnetic field can be formed by a current<br />

in a circuit, a current can be formed by moving a portion of a closed electric<br />

circuit through an external magnetic field, as indicated in Figure 22-1.<br />

The process of inducing a current in a circuit <strong>with</strong> a changing magnetic field<br />

is called electromagnetic induction.<br />

Consider a circuit consisting of only a resistor in the vicinity of a magnet.<br />

There is no battery to supply a current. If neither the magnet nor the circuit is<br />

moving <strong>with</strong> respect to the other, no current will be present in the circuit. But<br />

if the circuit moves toward or away from the magnet or the magnet moves<br />

toward or away from the circuit, a current is induced. As long as there is relative<br />

motion between the two, a current can form in the circuit.<br />

The separation of charges by the magnetic force induces an emf<br />

It may seem strange that there can be an induced emf <strong>and</strong> a corresponding<br />

induced current <strong>with</strong>out a battery or similar source of electrical energy. Recall<br />

that in the previous chapter a moving charge can be deflected by a magnetic<br />

field. This deflection can be used to explain how an emf occurs in a wire that<br />

moves through a magnetic field.<br />

100<br />

200<br />

300<br />

400<br />

500<br />

600<br />

700<br />

800<br />

900<br />

1000<br />

Galvanometer<br />

S<br />

<strong>Current</strong><br />

N<br />

Magnetic field<br />

Copyright © by Holt, Rinehart <strong>and</strong> Winston. All rights reserved.

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