Need help with centripetal acceleration questions

In summary: Will get back to you as soon as I can!In summary, for the first problem, the point on the top of the tire rim will be moving at a speed of 2at after 4.0 seconds, given that the cyclist is accelerating at a rate of 0.80 m/s^2 and the tire has a diameter of 68cm. For the second problem, the maximum speed at which a 1000kg car can round a turn of radius 100m on a flat road with a coefficient of friction of 0.5 is not dependent on the mass of the car, and can be calculated using Newton's 2nd law and the formula for centripetal acceleration.
  • #1
wikidrox
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1. A cyclist accelerates from rest at a rate of 0.80 m/s^2. How fast will a point on the top of the tire rim (diameter = 68cm) be moving after 4.0 s? (hint: At any given moment, the lowest point on the tire is in contact with the ground and hence is at rest.)

2. What is the max speed with which a 1000kg car can round a turn of radius 100m on a flat road if the coefficient of friction between the tires and road is 0.5? Is the result independent of the mass of the car?

I need some assistance on how to go about doing the questions. What equations do I use where?
 
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  • #2
For the first problem, find out how fast the cyclist is going after 4.0 s. (Use the equations for uniform accelerated motion.) Then figure out how fast the tire must be spinning since it rolls without slipping.

For the second problem, apply Newton's 2nd law. Since the car is going around a curve, the acceleration is centripetal. The only force is friction--the maximum force of friction is μmg.
 
  • #3
wikidrox said:
1. A cyclist accelerates from rest at a rate of 0.80 m/s^2. How fast will a point on the top of the tire rim (diameter = 68cm) be moving after 4.0 s? (hint: At any given moment, the lowest point on the tire is in contact with the ground and hence is at rest.)

First make a formula for the linear velocity of the cyclist, Vc is the velocity of the centre of the tire.

[tex]V_c = at[/tex]


Now find the rotation speed of the tire, assuming rotation around where the tire touches the ground.

[tex]V_c = \omega r[/tex]

[tex]\omega = \frac{V_c}{r}[/tex]

Fill in the equation above (for Vc)

[tex]\omega = \frac{at}{r}[/tex]

Now since you are looking at a point across the diameter of the tire, it's 2r distance away. let Va be the speed of the point at the top of the tire

[tex]V_a = \omega (2r)[/tex]

[tex]V_a = (\frac{at}{r})(2r)[/tex]

[tex]V_a = 2at[/tex]


2. What is the max speed with which a 1000kg car can round a turn of radius 100m on a flat road if the coefficient of friction between the tires and road is 0.5? Is the result independent of the mass of the car?

I'll have to think about this for a while, but I get the feeling it is not mass dependant.
 

FAQ: Need help with centripetal acceleration questions

1. What is centripetal acceleration and how is it different from regular acceleration?

Centripetal acceleration is the acceleration that an object experiences while moving in a circular motion. It is different from regular acceleration because it is always directed towards the center of the circle, while regular acceleration can be in any direction.

2. How is centripetal acceleration calculated?

Centripetal acceleration can be calculated using the formula a = v^2/r, where a is the centripetal acceleration, v is the velocity of the object, and r is the radius of the circular motion.

3. What are some real-life examples of centripetal acceleration?

Some real-life examples of centripetal acceleration include a car moving around a curve, a ball being swung around on a string, and a satellite orbiting around the Earth.

4. Can centripetal acceleration ever be negative?

No, centripetal acceleration is always positive because it is a measurement of the rate of change of velocity in a circular motion. Negative acceleration would mean that the object is slowing down, which is not possible in a circular motion.

5. How does centripetal acceleration affect the stability of an object?

Centripetal acceleration plays a crucial role in keeping an object stable in circular motion. It is responsible for constantly changing the direction of the object's velocity, which keeps it from flying off in a straight line. Without centripetal acceleration, the object would not be able to maintain a curved path and would instead continue moving in a straight line.

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