Finding Angular Velocity and Center of Mass Velocity for a Free Rotating Rod

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Homework Help Overview

The discussion revolves around a physics problem involving a free rotating rod subjected to an impulse. The original poster seeks to determine the angular velocity and the velocity of the center of mass after the impulse is applied. The context includes concepts from mechanics, specifically relating to angular momentum and impulse-momentum theorems.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of the impulse theorem and its implications for calculating angular velocity and center of mass velocity. There are questions about the completeness of the equations presented and whether the velocity of the center of mass is independent of the point of impulse application.

Discussion Status

Some participants have provided feedback on the equations and factors involved, while others have raised questions about the assumptions made regarding the center of mass and the effects of the applied impulse. There is an ongoing exploration of the relationship between the impulse applied and the resulting velocities.

Contextual Notes

Participants note the absence of friction and the specific conditions under which the impulse is applied, which may affect the outcomes being discussed. There is also mention of the need for clarity regarding the equations used in the calculations.

physicsisgreat
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Homework Statement


I have a rod of mass m and length l on a table without any kind of friction. I give it an impulse J in any point of distance d from the center of the rod, parallel to the table and perpendicular to the rod.
Find the angular velocity ω and the velocity of the center of mass v0.

Homework Equations


Moment of inertia of the rod rotating around its center: I = m l2 / 12
L = I · ω

The Attempt at a Solution


From the impulse theorem:
J = ΔP = P'
I can calculate ω from the angular momentum relations:
L = d x J = I · ω
ω = d J / I = 12 d J / (m l2),
which is 0 if I hit the rod on its center and max if I hit it on d = l/2.
Now I fail to calculate v0 :P

Thank you in advance :)
 
Last edited:
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Hello P.i.G., welcome to PF :)

Your relevant equation needs one or two colleagues: currently v0 doesn't feature there, ##\omega## doesn't, etc.

Your relevant equation also needs improvement. There is a factor missing.
 
Should you not apply a couple of equal torques (one clock and one anti-clock) to stop any motion of the centre of mass?
 
dean barry said:
Should you not apply a couple of equal torques (one clock and one anti-clock) to stop any motion of the centre of mass?
Not a good idea. 1. It doesn't work. 2. There is nothing that can be considered a cause for these ##\tau##. 3. The center of mass is not "stopped"
 
Hi, I edited my post adding the factor missing and an equation about ω (which I actually used later in my attempt at a solution).
I cannot give another equation about v0 though, as it is exactly what I am looking for! :)
 
Last edited:
Mmh, following the impulse-momentum theorem
J = ΔP
I would say that
v0 = J / m.

At the same time I wonder: can this be true? Can the velocity of the center of mass of the rod be independent from the point in which the impulse is applied?
 
physicsisgreat said:
Mmh, following the impulse-momentum theorem
J = ΔP
I would say that
v0 = J / m.

At the same time I wonder: can this be true? Can the velocity of the center of mass of the rod be independent from the point in which the impulse is applied?
Yes, it's correct. It feels wrong, until you realize that to impart the same impulse further from the centre of mass of the rod you have to 'work' harder. The rod tends to swing out of the way, so takes less momentum off the impacting object. To achieve the same imparted momentum the impacting object has to start with more momentum.
 
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Thank you very much haruspex! :)
 

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