Question

In: Physics

A stick is resting on a concrete step with 2/11 of its length hanging over the...

A stick is resting on a concrete step with 2/11 of its length hanging over the edge. A single ladybug lands on the end of the stick hanging over the edge, and the stick begins to tip. A moment later, a second, identical ladybug lands on the other end of the stick, which results in the stick coming momentarily to rest 56.9° from the horizontal. If the mass of each bug is 2.92 times the mass of the stick and the stick is 12.7 cm long, what is the magnitude of the angular acceleration of the stick at the instant shown?

Solutions

Expert Solution

Angular acceleration = (net torque) / (moment of inertia)
α = τ/I

Let L be the stick's length and let m be the stick's mass (so "2.92m" is each bug's mass). And let's say the "lower" ladybug is on the left. Then the lower ladybug exerts this much torque:

τ_lowerbug = −(2/11)L(2.92mg)cosθ (negative because I am (arbitrarily) choosing counter-clockwise as the negative angular direction).

The upper ladybug exerts this much torque:

τ_upperbug = +(9/11)L(2.92mg)cosθ

The weight of the stick can be assumed to act through its center, which is 7/22 of the way from the fulcrum. So the stick exerts this much torque:

τ_stick = +(7/22)L(mg)cosθ

The net torque is thus:

τ_net = τ_lowerbug + τ_upperbug + τ_stick
= −(2/11)L(2.92mg)cosθ + (9/11)L(2.92mg)cosθ + (7/22)L(mg)cosθ
= [(2.92x7/11)+(7/22)](mgL)cosθ = 2.176mgL(cosθ)

Now for the moments of inertia. The bugs can be considered point masses of "2.92m" each. So for each of them you can use the simple formula: I=mass×R²:

I_lowerbug = (2.92m)((2/11)L)² = (2.92m)(4/121)L²
I_upperbug = (2.92m)((9/11)L)² = (2.92m)(81/121)L²

For the stick, we can use the parallel axis theorem. This says, when rotating something about an axis offset a distance "R" from its center of mass, the moment of inertia is:

I = I_cm + mR²

We know that for a stick about its center of mass, I_cm is (1/12)mL² (see many sources). And in this problem we know that it's offset by R=(7/22)L. So:

I_stick = (1/12)mL² + m((7/22)L)²
= (1/12)mL² + (49/484)mL²
= 0.1845mL²

So the total moment of inertia is:

I_total = I_lowerbug + I_upperbug + I_stick
= (2.92m)(4/121)L² + (2.92m)(81/121)L² + (0.1845)mL²
= [2.92(4/121+81/121)+ 0.1845]mL² = 2.236mL2

So that means the angular acceleration is:

α = τ_net/I_total
= 2.176mgL(cosθ) / 2.236mL2 = 41 rad/s2


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