How Does Angular Velocity Influence Particle Motion in Rotational Dynamics?

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SUMMARY

The discussion focuses on the influence of angular velocity (ω) on the motion of a particle within a rotating tube. The particle, initially at a radial distance (a) from the axis, experiences no radial force as it slides without friction. The acceleration in the radial direction arises from the transformation of tangential velocity into a radial component, represented by the term ##r\dot\theta^2## in the radial equation. The equivalence of the centrifugal effect in a rotating coordinate system and the Coriolis effect on tangential force is also established.

PREREQUISITES
  • Understanding of angular velocity (ω) in rotational dynamics
  • Familiarity with curvilinear coordinates and their application
  • Knowledge of centrifugal and Coriolis forces
  • Basic principles of particle motion in a rotating frame
NEXT STEPS
  • Study the derivation of the radial equation in rotational dynamics
  • Explore the effects of Coriolis force in non-inertial reference frames
  • Learn about the application of curvilinear coordinates in physics
  • Investigate the relationship between angular velocity and radial acceleration
USEFUL FOR

Physics students, mechanical engineers, and anyone interested in the dynamics of particles in rotating systems will benefit from this discussion.

ensten
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A particle of mass m is inside a long, narrow tube which rotates
a constant angular velocity ω in the horizontal plane. (This means that you see the tube
from the top of the figure and not from the side.) At time t = 0 is the particle on the radial distance a from the rotational axis and the radial velocity is zero. Then begins the slide without friction. Determine the particle radial distance from the rotation axis and the horizontal normal force of the particle from the tube functions
of the time!Why is equation (10) found in this solution https://dl.dropboxusercontent.com/u/12645136/Losningar.pdf equal to 0?

If the particle moves from the center outwards isn't a force acting upon it in the radial direction? Hence giving it an acceleration in the same direction?
 
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I will write this in English since it is public, PM me if you would perfer an explanation in Swedish:

No, assuming you solve this in a fixed coordinate system, there is no force acting in the radial direction (there simply is nothing to provide such a force). The reason you will have acceleration in the radial direction is that you use curvilinear coordinates, resulting in that a velocity in the tangential direction is translated into a radial component as the particle moves. This is described by the ##r\dot\theta^2## term in the radial equation.

If you instead chose to use a rotating coordinate system, the very same term will be provided by the centrifugal effect and you end up with the same equation. The tangential force will now be balanced by the Coriolis effect.
 

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