Rotational Dynamics of a light cup

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SUMMARY

The discussion focuses on the physics of a light cup catching a ball from a board elevated at an angle theta. It establishes that the ball will lag behind the falling board when theta is less than 35.3 degrees. Additionally, it concludes that the ball will successfully fall into the cup when the board is supported at this limiting angle, with the cup positioned at Rc = (2L)/(3cos(theta)). The key equations utilized include angular acceleration and kinematic equations for motion.

PREREQUISITES
  • Understanding of rotational dynamics and angular acceleration
  • Familiarity with kinematic equations, specifically x = vot + 0.5at²
  • Knowledge of gravitational components in inclined planes
  • Basic principles of projectile motion
NEXT STEPS
  • Study the concept of angular acceleration in rotational dynamics
  • Learn about the effects of gravitational components on inclined planes
  • Explore advanced kinematic equations and their applications in physics
  • Investigate the principles of projectile motion and its relation to falling objects
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Students of physics, educators teaching mechanics, and anyone interested in understanding the dynamics of motion in inclined systems.

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Homework Statement



A common physics demonstration consists of a ball resting at the end of a board of length L that is elevated at an angle of theta with the horizontal. A light cup is attached to the board at Rc (Rc is a distance up the board from the bottom, it is not past the support stick) so that it will catch the ball when the support stick is suddenly removed. a) show that the ball will lag behind the falling board when theta < 35.3 and b) the ball will fall into the cup when the board is supported at this limiting angle and the cup is placed at
Rc = (2L)/(3cos[tex]\theta[/tex])

Homework Equations



[tex]\alpha[/tex]r = a
x = vot + .5at2

The Attempt at a Solution



The ball falls straight down from the end of the board, so I found the time that it takes with x = vot + .5at2 .Next I wanted to find the time it takes for the beam (and cup) to fall down, but I'm not sure how to do this. I tried using a component of gravity (gcos[tex]\theta[/tex]) as the tangential acceleration, but then I realized that this value changes as the beam falls. So, how do I approach this problem?
 
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Start by finding the angular acceleration of the stick as a function of angle.
 

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