A 200 g rubber ball is attached to a 1.0 m long string and released from an angle (theta). It swings down and at the very bottom has a perfectly elastic collision with a 1.0 kg block. The block is resting on a frictionless surface and is connected to a 20 cm long spring with spring constant 2000 N/m. After the collision, the spring compresses a maximum distance of 3.0 cm. From what angle was the ball released?
We know that the height the ball drops from is given as h = L*(1 - cos), so
Ep = mgh = mgL(1-cos) = 0.2kg * 9.8m/s2 * 1m * (1 - cos) = 1.96J * (1 - cos)
This is converted into Ek at the bottom of the arc:
Ek = 1.96J * (1 - cos) = ½mv² = 0.1kg * v2
v² = 19.6m2/s2 * (1 - cos)
v = 4.43m/s * sqrt(1 - cos)
Let K = sqrt(1 - cos).
B. initial momentum = mv = 0.2kg * 4.43m/s * K = 0.89kg·m/s * K
final momentum = 0.89kg·m/s * K = 0.2kg * u + 1kg * v
For a perfectly elastic collision, we know that
relative velocity of approach = relative velocity of separation, so
4.43m/s * K = v - u, or
v = u + 4.43m/s * K
Plug this into the momentum eqn:
0.89kg·m/s * K = 0.2kg * u + 1kg * (u + 4.43m/s * K)
0.89kg·m/s * K - 4.43kg·m/s * K = 1.2kg * u
u = -3.54kg·m/s * K / 1.2kg = -2.95m/s * K ---- velocity of ball
v = u + 4.43m/s * K = 1.48m/s * K -----------velocity of block
For the spring, Ep = 0.5*kx2 =0.5 * 2000N/m * (0.03m)2 = 0.9 J
So this must equal the initial Ek of the block:
0.9 J = 0.5*mv2 =0.5 * 1kg * (1.48m/s * K)2 = 1.1J * K2 = 1.1J * (1 - cos)
1 - cos = 0.81
cos = 0.19
= 79.040
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