ーこニI Figure 6.5 (Example 6.4) A car moves into the page and is round- ing a curve on a road banked at an angle 0 to the horizontal. When friction is neglected, the force that causes the centripetal acceleration and keeps the car moving in its cir- cular path is the horizontal com- ponent of the normal force.

Glencoe Physics: Principles and Problems, Student Edition
1st Edition
ISBN:9780078807213
Author:Paul W. Zitzewitz
Publisher:Paul W. Zitzewitz
Chapter6: Motion In Two Dimensions
Section6.2: Circular Motion
Problem 16PP
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A car rounds a banked curve as shown. The radius of curvature of the road is R, the banking angle is θ, and the coefficient of static friction is μs. (a) Determine the range of speeds the car can have without slipping up or down the road. (b) Find the minimum value for ms such that the minimum speed is zero.

ーこニI
Figure 6.5 (Example 6.4) A car
moves into the page and is round-
ing a curve on a road banked at an
angle 0 to the horizontal. When
friction is neglected, the force that
causes the centripetal acceleration
and keeps the car moving in its cir-
cular path is the horizontal com-
ponent of the normal force.
Transcribed Image Text:ーこニI Figure 6.5 (Example 6.4) A car moves into the page and is round- ing a curve on a road banked at an angle 0 to the horizontal. When friction is neglected, the force that causes the centripetal acceleration and keeps the car moving in its cir- cular path is the horizontal com- ponent of the normal force.
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