Rotational Motion of a bowling ball

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Homework Help Overview

The problem involves the rotational motion of a bowling ball that transitions from sliding to rolling. It examines the relationship between linear and angular accelerations, friction, and energy conservation in the context of rotational dynamics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss using energy conservation and torque equations to analyze the problem. There are attempts to derive angular acceleration and clarify the application of the parallel axis theorem. Questions arise regarding the correctness of the denominator in the angular acceleration formula.

Discussion Status

Participants are actively engaging with the problem, exploring different approaches such as torque and conservation of momentum. Some guidance has been offered regarding the use of the parallel axis theorem and the role of friction in generating torque. There is a recognition of the complexity involved in the energy conservation approach.

Contextual Notes

There is a mention of the initial conditions of the bowling ball, specifically that it starts with no rotational kinetic energy and the coefficient of friction is a key variable in the discussion. The distinction between the slipping and rolling phases is also noted.

PrettyLights
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Homework Statement


A bowling ball is released with speed V and no rotational kinetic energy. After a period of sliding and rotating, the ball enters pure rotational motion. The coefficient of friction between the ball and the ground while sliding is Uk.
a. Show that the rotational acceleration of the ball during the initial period of diluting is alpha=5gUk/2R, where g is the acceleration due to gravity and r is the radius of the ball (a solid sphere).
b. Show that when sliding finishes and rolling begins, the speed of the center of mass is Vc=5V/7

Homework Equations


Rotational Kinetic Energy= 1/2IW^2
Force due to friction= Ukmg
Kinetic Energy= 1/2mv^2

The Attempt at a Solution


I tried this problem from the angle of energy conservation but it quickly gets complicated. I tried to work from:
Potential energy of the ball + energy lost due to friction + Rotational energy = Total Kinetic, and then subbing in I and solving for V, plugging V into w=v/R and then l x V = alpha. Any help is appreciated.
 
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Have you tried using the torque equation?
Torque = I * alpha (Hint: use the parallel axis theorem and use the frictional force as the force producing the torque).
Conservation of energy can be used to get the final rotational speed, but
a very concise solution can be obtained using conservation of momentum.
You wrote alpha=5gUk/2R for the angular acceleration.
Are you sure the denominator should be 2 R and not 7 R.
 
My mistake - 2 R should be correct because the parallel axis theorem would not apply
while the ball is slipping, but it can be used when the ball reaches its final speed.
 
J Hann said:
the parallel axis theorem would not apply while the ball is slipping
To clarify, the difficulty with applying the parallel axis theorem while the ball is slipping is that the instantaneous centre of rotation is moving. It starts off infinitely below ground (i.e., not rotating) and finishes at ground level.
J Hann said:
a very concise solution can be obtained using conservation of momentum.
That's conservation of angular momentum, right?
 
Okay, so if I start with the equations for Torque this is where it takes me:

alpha=T/I = (F x R)/(2/5)MR^2 = Mguk x R/ (2/5)Mr^2 = 5guk/2R

This seems right to me because, as you said, the friction is the external force causing the torque. Thank you!
 
PrettyLights said:
Okay, so if I start with the equations for Torque this is where it takes me:

alpha=T/I = (F x R)/(2/5)MR^2 = Mguk x R/ (2/5)Mr^2 = 5guk/2R

This seems right to me because, as you said, the friction is the external force causing the torque. Thank you!
Looks right.
 

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