Mass falls on lever, catapulting mass on other end

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The discussion centers on a physics problem involving a catapult mechanism where a heavy mass drops onto a lever, launching a smaller mass at a 45-degree angle. Key considerations include the conservation of momentum during the inelastic collision between the putty and the lever, and the conversion of gravitational potential energy into rotational kinetic energy. Participants explore the equations governing energy and momentum to determine the distance the smaller mass lands from the launch point. The approach emphasizes the importance of correctly applying energy conservation principles and understanding the nature of the collision. The analysis concludes with a focus on deriving the angular velocity post-impact to solve for the launch distance.
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Homework Statement


You have constructed a simple catapult which basically consists of a 4 meter long rod of negligible mass attached to a fulcrum point offset from the center of mass by 1.5 meters. You decide to launch a m2 = 0.100 kg mass from the long end of the rod by dropping a m1 = 20.0 kg ball of putty from a height of h = 5 m onto the short side of the rod. The putty sticks to the rod when it hits it, causing the rod to rotate about the fulcrum until the short end of the rod hits the ground. At this point the small mass is launched into the air at an angle of 45 degrees. You may model the mass of putty and the small block as point particles. How far away from the launch point does the mass land when it hits the ground?

m1 = 20.0 kg
m2 = 0.100 kg
r1 = .5 m
r2 = 3.5 m
L = 4 m
h = 5 m
θ = 45°

Homework Equations





The Attempt at a Solution


In my solution, I assumed that no Kinetic Energy was lost during the collision and that the linear Kinetic Energy just translated into Rotational Kinetic Energy. So the rotational kinetic energy of mass 1 as it starts to rotate is equal to its change in GPE from falling. That was the part I was most unsure of.

I then used energy conservation to solve for ωf:

KA0 + UA0 + KB0 + UB0 = KAf + UAf + KBf + UBf
where A refers to mass 1, B refers to mass 2, t0 is the time of impact, and tf is the time of release

KAf + KBf = KA0 + UA0 + UB0 - UBf

Abstract away the known energies: let C = KA0 + UA0 + UB0 - UBf
KAf + KBf = C

.5mArA2ω2 + .5mBrB2ω2 = C

ω = √(2C/(mArA2 + mBrB2))
 
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The collision of the putty with the stick will probably be inelastic, so you don't want to assume that kinetic energy is conserved during the collision.

However, there's another quantity that you can argue is conserved during the collision.
 
TSny said:
The collision of the putty with the stick will probably be inelastic, so you don't want to assume that kinetic energy is conserved during the collision.

However, there's another quantity that you can argue is conserved during the collision.

It's momentum, right? vf = (m0 * v0)/mf
But what is mf?
 
Oh I think I get it now. mvr = (Ia + Ib)w
So once I find the angular velocity right after impact, the rest of my equations hold, right?
Total energy = Kinetic Energy + Gravitational Potential Energy?
 
Yes. Good!
 
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