Rotational Motion of a thin rod about a pivot

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Homework Help Overview

The discussion revolves around the rotational motion of a uniform thin rod pivoted at one end, focusing on its angular velocity when reaching a vertical position and the forces involved. The problem also explores the initial angular velocity required for the rod to swing through a specified angle.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of conservation of energy principles and the parallel-axis theorem. There is a specific focus on the reasoning behind the initial approach to part c and the validity of assumptions made.

Discussion Status

Some participants have provided insights into the connections between the different parts of the problem, particularly regarding the conservation of energy. There is an ongoing exploration of the implications of these connections, although not all participants agree on the interpretations.

Contextual Notes

Participants express uncertainty about the correctness of their initial assumptions and calculations, particularly in part c. There is mention of grading errors contributing to confusion, which may affect the clarity of the discussion.

WWCY
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Homework Statement


A uniform thin rod of Length L and mass M is pivoted at one end is held horizontally and then released from rest. Assuming the pivot to be frictionless, find

a) Angular velocity of the rod when it reaches its vertical position
b) The force exerted by the pivot at this time
c) Now we want to swing the rod 270° clockwise so that it will reach a vertical position at the top of its swing. What initial angular velocity is needed for the rod to achieve that?

Homework Equations


Part a)
Parallel-axis theorem
Conservation of Energy

Part b)
∑Fcm = mω2r

Part c)
Conservation of Energy?

The Attempt at a Solution


I actually have no issues with parts A and B but only with C.

My initial concept for C was to use the principle of COE
Ugrav, 1 + Krotational, 1 = Ugrav, 2
but this was wrong.

May I know what my concept for part c should be and why I was wrong in the first place?

P.s. Apologies if this post was not well done, it's my first post and feedback is appreciated. Thanks!
 
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WWCY said:
Part c)
Conservation of Ene
Ugrav, 1 + Krotational, 1 = Ugrav, 2
but this was wrong.

Why do you think it is wrong ?

Please show your calculations and result you obtained .
 
Having answered a, there is a very quick route to c.
 
Damn, apologies everyone, my initial assumptions were right. I got confused because of some grading error. Sorry for taking up your time!

In any case it was:

Ugrav1 + K rot 1 = Ugrav2
1/2Iω2 + mgL = mg(3/2)L
ω=(mgL/I)1/2
where I = 1/3mL2 with parallel axis theorem, which leads to:
ω = (3g/L)1/2 rads/s
 
WWCY said:
Damn, apologies everyone, my initial assumptions were right. I got confused because of some grading error. Sorry for taking up your time!

In any case it was:

Ugrav1 + K rot 1 = Ugrav2
1/2Iω2 + mgL = mg(3/2)L
ω=(mgL/I)1/2
where I = 1/3mL2 with parallel axis theorem, which leads to:
ω = (3g/L)1/2 rads/s
Right... and do you see the connection with the answer to a?
 
haruspex said:
Right... and do you see the connection with the answer to a?

Apart from them being the same, I can't. Could you enlighten me?
 
WWCY said:
Apart from them being the same, I can't. Could you enlighten me?
In both cases the potential difference relates to a rotation from horizontal to vertical, and in both cases it is stationary at one end of the motion, so the speeds at the other end must be the same.
 
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haruspex said:
In both cases the potential difference relates to a rotation from horizontal to vertical, and in both cases it is stationary at one end of the motion, so the speeds at the other end must be the same.

I never thought of it this way before, thank you for the insight.
 

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