Daniel B. answered 04/21/22
A retired computer professional to teach math, physics
Instead of making two calculations, one for each rod,
I will first calculate moment of inertia of a sphere attaching itself
to an arbitrary rod at an arbitrary spot.
Then I will apply the formula to the two cases.
The two cases can be distinguished by two numbers, let's call them p and q.
The number p (which is 2 in one case and 3 in the other) is the multiple of R
giving the length of the rod.
The number q (which is 2 in one case and 1.5 in the other) is the multiple of R
giving the distance of the sphere from the pivot.
Let
p and q be two numbers satisfying (0 < q ≤ p),
m be the mass of the sphere,
pm be the mass of the rod,
pR be the length of the rod,
qR be the distance from the pivot to where the sphere is attached,
v be the velocity with which the sphere strikes the rod.
I will make three assumptions with the justification that without these assumptions
the statement of the problem would be missing information.
Assumption 1: The rod has uniform density.
Assumption 2: The sphere's radius is so small that the sphere can be treated as single point.
Assumption 3: The pivot is at one end of the rod, opposite to where the sphere attaches to the shorter rod.
Once the rod with the sphere starts rotating, the angular momentum is
L = Iω
where
I is the moment of inertial of the combination rod + sphere,
ω is angular velocity.
We need to compute both I and ω.
The moment of inertia I = Ir + Is, where
Ir is the moment of inertia of the rod and Is is the moment of inertia of the sphere.
By Assumption 1,
Ir = pm(pR)²/2
By Assumption 2,
Is = m(qR)²
So
I = pm(pR)²/2 + m(qR)² = mR²(p³/2 + q²)
The angular velocity ω can be obtained from conservation of energy.
Before the collision, the energy of the system consists of kinetic energy of the sphere:
mv²/2
After the collision, the energy of the system is the rotational energy:
Iω²/2
Therefore the two must be equal
Iω²/2 = mv²/2
So
ω = v√(m/I)
Now we can express the angular momentum
L = Iω = Iv√(m/I) = v√(mI) = v√(m²R²(p³/2 + q²)) = vmR√(p³/2 + q²)
Now we can come back to having the two situations characterized by different p and q
Shorter rod: p1 = 2, q1 = 2
Longer rod: p2 = 3, q2 = 1.5
L1 : L2 = √(p1³/2 + q1²) / √(p2³/2 + q2²)
= √((p1³ + 2q1²) / (p2³ + 2q2²))
= √((2³ + 2×2²) / (3³ + 2×1.5²)) ≈ 0.71