Conservation of angular momentum of a thin rod

AI Thread Summary
The discussion revolves around a physics problem involving the conservation of angular momentum when a clay ball strikes a thin rod. Participants clarify the use of the moment of inertia (I) for both the rod and the clay, emphasizing the importance of determining the new center of mass after the collision. They discuss the application of angular momentum conservation about different points, noting that it can be measured from any point, not just the center of mass. The conversation highlights the calculation of angular momentum for both the clay and the rod separately, suggesting this approach may simplify the problem. Ultimately, the participants aim to derive the correct equations to analyze the translational and rotational motions post-collision.
xfreedom
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Homework Statement



A thin rod of mass M and length L rests on a frictionless table and is struck L/4 from its CM by a clay ball of mass m moving at speed v. The ball sticks to the rod. Determine the translational and rotational motion

Homework Equations


Irod=1/12 mr^2
Irod=1/3 mr^2
L=mrv=Iw

The Attempt at a Solution


I fount out the translational velocity, used the conservation of linear momentum.
But I'm kind of stop in the second part.
I found out:
m(1/4 l)v=Iw
but what is I?
I guess perhaps we needs to find out the new center of mass, is it (1/12 Ml^2)+(mr^2) where r is calculated with the new center of mass? Is it(m 1/4 l)/(M+m)? And again which Irod should I use?

thank you for help.
 
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hi xfreedom! welcome to pf! :smile:
xfreedom said:
… but what is I?
I guess perhaps we needs to find out the new center of mass, is it (1/12 Ml^2)+(mr^2) where r is calculated with the new center of mass? Is it(m 1/4 l)/(M+m)? And again which Irod should I use?

for conservation of angular momentum, you can measure angular momentum about any point

(it is only for τ = Iα that you are restricted to the centre of mass or centre of rotation)

so you may as well use the centre of mass of the rod itself :wink:
 
tiny-tim said:
hi xfreedom! welcome to pf! :smile:


for conservation of angular momentum, you can measure angular momentum about any point

(it is only for τ = Iα that you are restricted to the centre of mass or centre of rotation)

so you may as well use the centre of mass of the rod itself :wink:


Thanks for your reply.
So just to be sure, is the correct formula should be

m(1/4 l)v=Iw

where I equal to 1/12 ML^2 + [(m 1/4 l)/(M+m)-1/4 l]^2 m?

thank you.
 
hi xfreedom! :smile:
xfreedom said:
… where I equal to 1/12 ML^2 + [(m 1/4 l)/(M+m)-1/4 l]^2 m?

(isn't that second term negative? :redface:)

no, the second term is just the moment of inertia of the clay at a distance L/4

(and now I'm off to bed :zzz:)
 
tiny-tim said:
hi xfreedom! :smile:


(isn't that second term negative? :redface:)

no, the second term is just the moment of inertia of the clay at a distance L/4

(and now I'm off to bed :zzz:)


...and I believe the clay and the rod will rotate with the new center of mass? So the I for clay should be the distance between the clay and the new CM?

Thank you.

And have a good dream lol
 
hi xfreedom! :smile:

i'll expand on my original post (it's too late to edit it), in case you'e not clear about what formula to use:

for conservation of angular momentum, we can measure angular momentum L about any point P

provided we use the full formula LP = Ic.o.mω + mrc.o.m x vc.o.m

(it is only for LP = IPω (and τP = IPα) that we are restricted to P being the centre of mass or centre of rotation)

so you may as well use the centre of mass of the rod itself :wink:

xfreedom said:
...and I believe the clay and the rod will rotate with the new center of mass?

it depends what you mean

the centre of rotation is well below the centre of mass …

that is (by definition) the point about which the clay and the rod rotate

but if you mean, do you use the new centre of mass to calculate the angular momentum of the clay-and-rod, the answer is yes

(but why do that when it's easier to calculate the two individual angular momentums, and then add them?)
So the I for clay should be the distance between the clay and the new CM?

(I ? :confused:)

as i said, you can use any point P

if you use the centre of mass, you get m(u-v)R = Iω

if you use a point distance d above the centre of mass, you get m(u-v)(R-d) = Iω - MVd

subtracting those, and dividing by d, gives m(u-v) = MV …

which is automatically true, since it's the equation for conservation of ordinary momentum! :wink:

finally, instead of the centre of mass, you might in this case find it more convenient to use the point of impact as P, since that gives you ω independently of the masses :smile:
 
Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
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