Conservation of angular momentum of a thin rod

In summary, the problem involves a thin rod of mass M and length L being struck by a clay ball of mass m moving at speed v and sticking to the rod. The goal is to determine the translational and rotational motion of the system. Using the conservation of linear momentum, the translational velocity can be found. To find the angular momentum, any point can be used as the center of rotation, but it is more convenient to use the center of mass of the rod itself. The moment of inertia for the clay can be calculated using the distance between the clay and the center of mass. Alternatively, the point of impact can be used as the center of rotation to find the angular velocity independent of the masses.
  • #1
xfreedom
3
0

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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  • #2
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:
 
  • #3
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.
 
  • #4
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:)
 
  • #5
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
 
  • #6
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:
 

1. What is conservation of angular momentum?

Conservation of angular momentum is a fundamental law of physics that states that the total angular momentum of a closed system remains constant, unless acted upon by an external torque.

2. How does angular momentum relate to a thin rod?

In the context of a thin rod, conservation of angular momentum means that the total angular momentum of the rod (considering both its linear and rotational motion) will remain constant as long as there is no external torque acting on it.

3. What is the formula for calculating angular momentum of a thin rod?

The formula for angular momentum of a thin rod is L = Iω, where L is the angular momentum, I is the moment of inertia, and ω is the angular velocity of the rod.

4. How does conservation of angular momentum apply to rotational motion of a thin rod?

In rotational motion, the angular momentum of a thin rod is conserved as long as there is no external torque acting on it. This means that the rod will continue to rotate at a constant rate unless an external force (such as friction) causes it to slow down.

5. What are some real-life applications of conservation of angular momentum of a thin rod?

Conservation of angular momentum is a crucial concept in many fields, including astrophysics, engineering, and sports. For example, it explains the stability of spinning objects such as tops and gyroscopes, the motion of planets and satellites in orbit, and the conservation of energy in fluid dynamics.

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