Rotational Mechanics & Collisions question

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Homework Help Overview

The problem involves a meter stick pivoted at one end with a mass attached to it, exploring the dynamics of a collision and subsequent motion. The subject area includes rotational mechanics and inelastic collisions.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants discuss the conservation of momentum and energy during the collision and subsequent motion of the system. There are attempts to calculate angular momentum before and after the collision, as well as considerations of the center of mass and gravitational potential energy.

Discussion Status

Some participants have offered hints regarding the conservation of angular momentum and energy, while others are questioning the assumptions made about forces and torques involved in the system. Multiple interpretations of the problem are being explored, particularly concerning the calculations of angular momentum and moment of inertia.

Contextual Notes

There are indications of confusion regarding the effects of the pivot on momentum conservation and the calculation of the moment of inertia for the combined system of the rod and mass. Participants are also grappling with discrepancies in their results for the angle of displacement.

rohanprabhu
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Homework Statement


Q] A meter stick weighing 240 grams is pivoted at it's upper end in such a way that it can freely rotate through this end. A particle of mass 100 gms is attached to the upper end of the stick to a string of length 1m. Initially the rod is kept vertical and the string horizontal when the system is released from rest. The particle collides with the lower end of the stick and sticks there. Find the maximum angle through which the stick will rise.

http://img110.imageshack.us/img110/2136/img1vd2.png

The Attempt at a Solution



This is a case of pure inelastic collision. In this case:

[tex] \Delta {mv} = 0[/tex]

The potential energy of the particle at the position in rest is 1J. Hence, when it reaches the bottom, it's P.E will get converted to K.E. Hence:

[tex] \frac{1}{2}mv^2 = 1[/tex]

and hence,

[tex] v = \sqrt{2}{m} = \sqrt{20} = 2\sqrt{5}[/tex]

and the momentum is given by:

[tex] p = mv = 0.2\sqrt{5}[/tex]

Now, when it collides with the rod below, the momentum of the whole system at this point will be the same, but the mass of the system is now 0.24 + 0.1 = 0.34 gms. Hence, the velocity of the system at this point is given as:

[tex] v = \frac{0.2\sqrt{5}}{0.34}[/tex]

Now, the situation can be simplified to: There is a system of a bob attached to a rod, with:

[tex] I = 0.24~ kgm^2~~;~~m = 0.34 ~kg[/tex]

A gravitational force acts on it and i am left to determine by how much the system will be displaced [angular] under this force. I have no idea how to do that as of now. Any help is appreciated.
 
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Comments:
(1) During the collision: Since the stick is constrained by its pivot, translational momentum is not conserved. But what is?
(2) After the collision: Energy is conserved as the stick+mass swings up. Hint: Where's the center of mass?
 
Doc Al said:
Comments:
(1) During the collision: Since the stick is constrained by its pivot, translational momentum is not conserved. But what is?
(2) After the collision: Energy is conserved as the stick+mass swings up. Hint: Where's the center of mass?

I did not realize the external force by the pivot. However, the pivot will exert a force along the rod and hence the torque will be zero [i guess]. So, will the angular momentum stay constant?
 
rohanprabhu said:
So, will the angular momentum stay constant?
Exactly.
 
I tried doing it using conservation of angular momentum now. Just before the bob strikes the rod, it's angular momentum is given by:

[tex] l = mvr= (0.1)(2\sqrt{5})(1) = 0.2\sqrt{5}[/tex]

After collision, the angular momentum of the system will remain constant. Hence,
[tex] I\omega = 0.2\sqrt{5}[/tex]

[tex] \omega = \sqrt{5}{1.2}[/tex]

The K.E. of the system at this point is given as:

[tex] K.E = \frac{1}{2}I\omega^2 = \frac{10}{24}[/tex]

The center of mass is at a distance 'r' from the pivoted end:

[tex] r = \frac{1}{0.34}[(0.24)(0.5) + (0.1)(1)} = \frac{11}{17}[/tex]

At this point, the gravitational force will be acting. The perpendicular distance of this point from where we computed the K.E is given [or took the P.E to be zero] is given by:

[tex] h = 1 - \frac{11}{17}cos(\theta)[/tex]

On equating the GPE at this point with the K.E found earlier, i am getting the theta as ArcCos[0.9], whereas i should be getting ArcCos[0.75]. What am i doing wrong here?
 
What are you using for the rotational inertia of rod + mass?
 
how we can find the moment of inertia of aflywheel peactically , you don,t know the mass of flywheel and also consider friction?
 

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