Bowling Ball Slipping and Rolling: Analyzing Acceleration

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SUMMARY

The discussion focuses on the dynamics of a uniform, spherical bowling ball projected horizontally with an initial velocity of 6.00 m/s. The ball transitions from slipping to rolling without slipping due to kinetic friction, characterized by a coefficient μk. Key equations derived include the linear acceleration a, which is negative as the ball slows down, and the angular acceleration α, which is determined using torque and moment of inertia. The condition for rolling without slipping at the transition time ts is that the linear velocity v and angular velocity ω must satisfy the relationship v = Rω.

PREREQUISITES
  • Understanding of Newton's 2nd law for translation and rotation
  • Familiarity with the concepts of linear and angular acceleration
  • Knowledge of frictional forces and their effects on motion
  • Basic principles of rotational dynamics, including torque and moment of inertia
NEXT STEPS
  • Study the derivation of linear acceleration in systems with friction
  • Learn about the relationship between linear and angular velocities in rolling motion
  • Explore the effects of different coefficients of friction on motion dynamics
  • Investigate the principles of rolling motion in various physical contexts
USEFUL FOR

This discussion is beneficial for physics students, mechanical engineers, and anyone interested in the mechanics of motion, particularly in understanding the transition between slipping and rolling in rigid bodies.

jnimagine
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A uniform, spherical bowling ball of mass m and radius R is projected horizontally along the
floor at an initial velocity v0 = 6.00 m/s. The ball is not rotating initially, so w0 = 0. It
picks up rotation due to (kinetic) friction as it initially slips along the floor. The coefficient of
kinetic friction between the ball and the floor is μk. After a time ts, the ball stops slipping and makes a transition to rolling without slipping at angular speed ws and translational velocity _s. Thereafter, it rolls without slipping at constant velocity.

(b) Find an equation for the linear acceleration a of the ball during this time. The acceleration should be negative, since the ball is slowing down.
(c) Find an equation for the angular acceleration a of the ball while it is slipping. It will be
simpler if you use the sign convention that clockwise rotations are positive, so > 0.
(d) What constraint on w and v must take effect at time t = ts, the moment when the ball
stops slipping and begins rolling without slipping?

Here is my attempt:
b) slipping = rw + deltavt = vt
and then you get a derivative of it to get a = u_kg
c) a = torque / I
r(ru_kmg / 2/5mr^2) + dv/dt = -u_kg
and we get like -7/2u_kg from this...
d)...

please help!
 
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Friction is the only horizontal force acting on the ball. Use Newton's 2nd law for translation and rotation to find the linear and angular accelerations.

For (d), what's the condition for rolling without slipping?
 

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