- #1
Justin428
Homework Statement
I have been thinking about this problem for comparison of experimental data to theoretical for a project.
A hammer with known mass mh and mass moment of inertia Ih is held stationary at 90 degrees. It is released as swings down. At 0 degrees it impacts a block, initially at rest, with known mass mb and mass moment of inertia Ib at a distance P from the center of mass. The block begins to rotate and translate across a frictionless plane perpendicular to the plane in which the hammer rotates. Assume perfectly elastic collision and no friction in the system. What is the final angular velocity of the hammer, final angular velocity of the block, and final transnational velocity of the block?
(See attachment for drawing)
u,i indicates initial velocity
v,f indicates final velocity
subscript h is for hammer
subscript b is for block
Homework Equations
Conservation of Momentum: mhuh + mbub = mhvh + mbvb
Conservation of angular momentum: Ihωh = Ibωb
Conservation of Energy: 0.5Ihωh2 = 0.5Ibωb2
The Attempt at a Solution
Initially, I attempted to solve to problem by starting with the PE of the hammer and and converting it to KE as it swings down. This gives me a tangential velocity at impact with the block. However, this does not account for the energy that remains in the hammer as it continues to swing up after impact and also assumes that the weight of the handle is negligible.
Next, I attempted to combine the conservation equations:
1.) PE to KE
mhgh = 0.5Ihωhi2
2.) Energy of hammer just before impact = block energy + energy of hammer after impact
0.5Ihωhi2 = 0.5mbvb2 + 0.5Ibωb2 + 0.5Ihωhf2
3.) Conservation of angular Momentum
Ihωhi = Ihωhf + Ibωb + (how to account for the linear momentum of block??)
*not sure out to account for the linear momentum of the block since substituting v = ωr does not reduce to the correct units. I believe I also need to incorporate the distance P to reduce the mass of the block to mb = mbkb/P2, where k is the radius of gyration.