Static Friction in Circular Motion

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The discussion focuses on calculating static friction in circular motion with a radius of 3.0 m and a coefficient of static friction of 0.28. The normal force is determined to equal the gravitational force, leading to the calculation of static friction and acceleration, resulting in an acceleration of 2.744 m/s². The time for one revolution is calculated to be 6.57 seconds, with the conclusion that mass does not affect this time. The direction of the frictional force is clarified to point towards the center of the circular path.
Softwarm
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Homework Statement
You are sitting on the edge of a horizontal disk (for example, a playground merry-go-round) that has radius 3.00 m and is rotating at a constant rate about a vertical axis. The coefficient of static friction between you and the surface of the disk is 0.280

A) What is the minimum time for one revolution of the disk if you are not to slide off? Express your answer with the appropriate units.

B) Your friend's weight is half yours. If the coefficient of static friction for him is the same as for you, what is the minimum time for one revolution if he is not to slide off? Express your answer with the appropriate units.
Relevant Equations
a = 4*π^2*r / T^2
A) So we are given the radius and the coefficient of static friction as 3.0 m and 0.28 respectively. I know that in the vertical direction the only forces acting are the normal force and the gravitational force. Therefore, the normal force is equal to mg because net force is equal to 0, due to no vertical acceleration.

I can find the force of static friction, FS = FN * μS
Net force in the horizontal direction, ma = FS, the only force is the force of friction
ma = mg * μS
a = g * 0.28
a = 2.744 m/s2

I'm not entirely sure where the frictional force would point on a free-body diagram but, I can use the acceleration to solve for the time for one revolution (T) with the equation mentioned above.

2.744 = 4 * π2 * (3) / T2
T = √(4 * π2 * (3) / 2.744)
T = 6.57 s

B) For this part, I don't think the differences in mass will have an affect on the time for one revolution.
When solving for the acceleration,
0.5m * a = 0.5m * g * μS
The 0.5m will just cancel out and we'll be left with the same acceleration and the same time for one revolution.
T = 6.57 s

Is my answer correct? I'm not sure if there is anything I missed or if I used my equations incorrectly.
 
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Welcome to PF!

Your work looks good. I think your answers for (a) and (b) are correct.

Softwarm said:
I'm not entirely sure where the frictional force would point on a free-body diagram
Whenever an object moves in a circle at constant speed, what is the direction of the net force acting on the object? Therefore, what must be the direction of the friction force in this problem?
 
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Softwarm said:
FS = FN * μS
Only in the limiting case, where it is on the verge of slipping (as here).
 
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TSny said:
Welcome to PF!

Your work looks good. I think your answers for (a) and (b) are correct.Whenever an object moves in a circle at constant speed, what is the direction of the net force acting on the object? Therefore, what must be the direction of the friction force in this problem?

Ahh I see, so it would point towards the center. Thanks.
 
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The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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