Rotational motion, frictionless.

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SUMMARY

The discussion centers on the dynamics of a cylinder with a mass of 4 kg and a moment of inertia (I) of 0.02 kg·m², wound with a rope and placed on a frictionless surface. It concludes that the cylinder accelerates linearly at 5.0 m/s² without rotation when friction is negligible. The equation Fr = Iα remains applicable, as angular and linear accelerations can be computed separately in the absence of friction. Additionally, a yo-yo in a zero-gravity environment will behave similarly, accelerating and spinning in the direction of the applied force.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Familiarity with rotational dynamics concepts, including moment of inertia
  • Knowledge of linear and angular acceleration relationships
  • Basic principles of motion in a frictionless environment
NEXT STEPS
  • Study the relationship between linear and angular motion in non-frictional systems
  • Explore the concept of instantaneous center of rotation in rigid body dynamics
  • Investigate the effects of friction on rolling motion and acceleration
  • Examine the behavior of objects in microgravity environments, focusing on rotational dynamics
USEFUL FOR

Physics students, mechanical engineers, and anyone interested in understanding the principles of rotational motion and dynamics in frictionless environments.

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http://img444.imageshack.us/img444/8148/rollwx.jpg

A rope is wound around a cylinder of mass 4kg, and I=0.02kg.m2 about the cylinder axis.
The frictional force between table and cylinder is negligible.

Solution:
a=20/4=5.0m/s2
α=ar is not applicable when slippage occurs.


My question.
1.Is the cylinder moves forward with acceleration a without any rotation.
2. Is Fr=Iα is still applicable in this case, even though we know α=ar not applicable.
3. If we play yo-yo in zero gravity environment,how does the yo-yo behave when we pull it?

Thank you.
 
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1. No, see 2.
2. Yes, Fr=Iα is always applicable. α=ar constraint is only needed for rolling, and is achieved via additional force, that being the force of friction. When no friction is present, you just compute angular and linear accelerations separately.
3. Yo-yo in zero-g will behave exactly the same as this test case. It will accelerate and spin in direction it's being pulled.
 
Thank you.
That really helpful since the book didn't say about rotation only a=αr is not applicable.
 
A nice question to ask here is to find the instantaneous centre of rotation.
 

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