Two 2.00kg balls are attached to the ends of a thin rod length 50.0cm and negligible mass. The rod is free to rotate about a horizontal axis at the center, without friction. With the rod horizontal, a 50.0 gram glob of putty drops onto one of the balls, hitting it with a speed of 3.00m/s and sticking to it.

What is the angular velocity of the system just after the wad hits and sticks?

I'm supposed to use conservation of angular momentum to solve this.

To solve this problem using the conservation of angular momentum, we need to consider the initial and final states of the system.

Initially, the system consists of two balls attached to a rod, with no external forces acting on it. Since the rod is free to rotate without friction, the initial angular momentum of the system is zero because the balls are at rest.

When the 50.0 gram glob of putty drops onto one of the balls and sticks, it imparts angular momentum to the system. The angular momentum of a particle can be calculated using the equation:

L = mvr

Where:
L = angular momentum
m = mass
v = linear velocity
r = perpendicular distance from the axis of rotation

In this case, the glob of putty hits the ball with a speed of 3.00 m/s. Since the ball is attached to the rod and the rod is free to rotate about its center, the perpendicular distance from the axis of rotation is the length of the rod divided by 2 (25.0 cm or 0.25 m).

So, the angular momentum imparted by the glob of putty to the ball can be calculated as:

L1 = m1 * v * r1

Where:
m1 = mass of the ball
v = velocity of the putty
r1 = perpendicular distance from the axis of rotation for the ball

Next, to ensure conservation of angular momentum when the glob of putty sticks to the ball, an equal and opposite angular momentum should be imparted to the combined system of the ball, putty, and the other ball.

Since the two balls are symmetric, the perpendicular distance from the axis of rotation for the second ball is also 0.25 m, and the angular momentum imparted to the second ball can be calculated as:

L2 = m2 * v * r2

Where:
m2 = mass of the second ball
v = velocity of the putty
r2 = perpendicular distance from the axis of rotation for the second ball

According to the conservation of angular momentum, the sum of the initial angular momentum (zero) and the angular momentum imparted by the putty to the two balls should be equal to the final angular momentum.

L_initial + L1 + L2 = L_final

Since the final state is the system with the glob of putty stuck to one of the balls, the moment of inertia of the system changes. The moment of inertia, I, for a system of two balls rotating about a central axis is given by:

I = I1 + I2

Where:
I1 = moment of inertia of the ball with putty stuck to it
I2 = moment of inertia of the second ball

The moment of inertia for a ball can be calculated using the equation:

I = (2/5) * m * r^2

Where:
m = mass of the ball
r = radius of the ball

The moment of inertia for the system of the ball with putty and the second ball can be calculated by adding the individual moments of inertia.

Once we have the moment of inertia for the final system, we can rearrange the conservation of angular momentum equation to solve for the final angular velocity, ω.

L_final = I * ω_final

Plugging in the values and solving the equation will give us the required angular velocity of the system just after the putty sticks to the ball.