What Are the Dynamics of a Collar Sliding on a Rotating Rod?

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SUMMARY

The discussion focuses on the dynamics of a 3-lb collar sliding on a rotating rod, specifically analyzing the radial and transverse components of acceleration at point A, the acceleration of the collar relative to the rod, and the transverse component of the collar's velocity at point B. The results indicate that the radial acceleration (Ar) and transverse acceleration (Aθ) at point A are both zero, while the acceleration of the collar relative to the rod is 1536 in/s² and the transverse velocity at point B is 32.0 in/s. The key concept emphasized is the application of Newton's second law to determine the forces acting on the collar without needing the radial position as a function of time.

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negatifzeo
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Homework Statement


A 3-lb collar can slide on a horizontal rod which is free to rotate about a vertical shaft. The collar is intially held at A by a cord attached to the shaft. A spring constant of 2 lb/ft is attached to the collar and to the shaft and is undeformed when the collar is at A. As the rod rotates at the rate ThetaDot=16 rad/s, the cord is cut and the collar moves out along the rod. Neglecting friction and mass of the rod, determine

a)the radial and transverse components of the acceleration at A

b)The acceleration of the collar relative to the rod at A

c)the transverse component of the velocity of the collar at B


Homework Equations





The Attempt at a Solution


I know the solution to the problem. The answers are
a) Ar=0, Atheta=0

b)1536 in./s^2

c)32.0 in/s

I don't feel like this is a difficult problem, but I am definitely missing a key concept. How can you determine these quantities without r as a function of time?
 

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Hi negatifzeo! :smile:

(have a theta: θ and an omega: ω and try using the X2 tag just above the Reply box :wink:)
negatifzeo said:
I don't feel like this is a difficult problem, but I am definitely missing a key concept. How can you determine these quantities without r as a function of time?

I suppose you're wondering how you can find r'' without knowing r(t)? :redface:

It doesn't matter, because you can work it out from good ol' Newton's second law … Fradial = m(r'' - ω2r) :wink:
 
tiny-tim said:
Hi negatifzeo! :smile:

(have a theta: θ and an omega: ω and try using the X2 tag just above the Reply box :wink:)


I suppose you're wondering how you can find r'' without knowing r(t)? :redface:

It doesn't matter, because you can work it out from good ol' Newton's second law … Fradial = m(r'' - ω2r) :wink:


The angular velocity is given. The mass is given. But we don't know the total force, do we? The total force is broken up into two components, "e-sub-r" and "e-sub-theta", which we do not know.
 
Hi negatifzeo! :smile:

(what hapened to that θ i gave you? :redface:)
negatifzeo said:
The angular velocity is given. The mass is given. But we don't know the total force, do we? The total force is broken up into two components, "e-sub-r" and "e-sub-theta", which we do not know.

You won't need the eθ component of the force.

Try it for a) first. :smile:
 

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