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Physics Solutions Manual

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Chapter 24 continued<br />

Challenge Problem<br />

page 656<br />

The figure shows two identical motors with a<br />

common shaft. For simplicity, the commutators<br />

are not shown. Each armature coil consists of<br />

48 turns of wire with rectangular dimensions of<br />

17 cm wide by 35 cm deep. The armature<br />

resistance is 12 . The red wire travels to the left<br />

(along half the width) and then back to the rear<br />

of the motor (along the depth). The magnetic<br />

field is 0.21 T. The diameter of the pulley is<br />

7.2 cm. A rope fixed to the pulley and the floor<br />

prevents the motor shaft from turning.<br />

Pulley<br />

S<br />

Spring<br />

scale<br />

S 1<br />

S<br />

Shaft<br />

N<br />

120 V<br />

1. Given F ILB, derive an equation for the<br />

torque on the armature for the position<br />

shown.<br />

Torque is defined as the product of the<br />

force and the lever arm. In the case of<br />

the motor armature position shown, the<br />

lever arm is equal to half of the width of<br />

the armature coil (the shaft is the center<br />

of rotation and is at the midpoint of the<br />

coil width). The length of the wire acted<br />

upon by the field is equal to the depth<br />

of the coil. This length is effectively<br />

increased by n, the number of turns in<br />

the coil. Finally, the torque is doubled<br />

because as one side is pushed up by<br />

the magnetic field, the other side is<br />

pushed down according to the third<br />

right-hand rule.<br />

2nBI(depth)(width/2)<br />

S 2<br />

N<br />

35 V<br />

Simplifying and replacing (depth)(width)<br />

with area, A, gives:<br />

nBIA<br />

The torque produced by the motor<br />

armature, in the position shown, is<br />

equal to the number of turns times the<br />

field strength times the armature current<br />

times the area of the armature coil.<br />

2. With S 1 closed and S 2 open, determine the<br />

torque on the shaft and the force on the<br />

spring scale.<br />

nBIA<br />

(48)(0.21 T)1 20<br />

V<br />

(0.35 m)(0.17 m)<br />

12<br />

<br />

6.0 Nm<br />

Because the shaft cannot turn, the system<br />

is in equilibrium and the force on<br />

the spring scale is found by considering<br />

half the pulley diameter:<br />

6.<br />

0 Nm<br />

Fspring scale 170 N<br />

0.<br />

036<br />

m<br />

3. With both switches closed, determine the<br />

torque on the shaft and the force on the<br />

spring scale.<br />

Both motors produce counterclockwise<br />

torque:<br />

1 (48)(0.21 T)1 20<br />

V<br />

(0.35 m)(0.17 m)<br />

12<br />

<br />

6.0 Nm<br />

2 (48)(0.21 T) 35<br />

V<br />

(0.35 m)(0.17 m)<br />

12<br />

<br />

1.7 Nm<br />

net 7.7 Nm counterclockwise<br />

7.<br />

7 Nm<br />

Fspring scale 210 N<br />

0.<br />

036<br />

m<br />

4. What happens to torque if the armature is<br />

in a different position?<br />

The torque is reduced when there is<br />

any rotation from the position shown<br />

because the lever arm is reduced. With<br />

90° rotation, the force on the armature<br />

will be up and down (canceling) with<br />

the effective lever arm equal to zero.<br />

With the shown position as 0°:<br />

nBIA cos <br />

500 <strong>Solutions</strong> <strong>Manual</strong> <strong>Physics</strong>: Principles and Problems<br />

Copyright © Glencoe/McGraw-Hill, a division of The McGraw-Hill Companies, Inc.

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