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This is from Kaplan's high yield problem solving guide:
"A car rounds a curve with a constant velocity of 25 m/s. The curve is a circle of radius 40 m. What must the coefficient of static friction between the road and the wheels be to keep the car from slipping?"
First, isn't it true that when a car is going around a curve, there's no way it can have constant velocity because the direction is constantly changing, but it can have constant speed. Right?
Second, they have you draw a free body diagram with the direction of the frictional force pointing towards the center of the circle. I thought that centripetal force pointed in this direction, and that the frictional force and centripetal force are two different forces entirely.
The problem is easy once I set the frictional force equal to m v^2/r. But where did the centripetal force go, and how did they figure out the direction of the frictional force.
"A car rounds a curve with a constant velocity of 25 m/s. The curve is a circle of radius 40 m. What must the coefficient of static friction between the road and the wheels be to keep the car from slipping?"
First, isn't it true that when a car is going around a curve, there's no way it can have constant velocity because the direction is constantly changing, but it can have constant speed. Right?
Second, they have you draw a free body diagram with the direction of the frictional force pointing towards the center of the circle. I thought that centripetal force pointed in this direction, and that the frictional force and centripetal force are two different forces entirely.
The problem is easy once I set the frictional force equal to m v^2/r. But where did the centripetal force go, and how did they figure out the direction of the frictional force.