2018 A/L Physics Past Paper · Question 34 (English Medium)

A spider landing on a rotating disc — L and ω of the disc

A disc freely rotates without friction at a certain angular speed, about a fixed vertical axis normal to the plane of the disc and passing through its centre. At time t=0t = 0, a spider vertically lowers itself with negligible speed onto the rim of the rotating disc as shown in figure, and becomes rest. Variation of the magnitudes of the angular momentum (L)(L) and the angular speed (ω)(\omega) of the disc only with time (t)(t) is best represented by,

  1. (1) Figure (1)
  2. (2) Figure (2)
  3. (3) Figure (3)
  4. (4) Figure (4)
  5. (5) Figure (5)
Answer and explanation

Answer: (3) Figure (3)

What the question asks

We want: the graph of LL and ω\omega of the disc only, before and after the spider lands.

Relevant theory

The total angular momentum of a system remains constant provided no external torque acts on the system.

The angular momentum (L) of a lamina moving with an angular velocity ω\omega about an axis passing through O is given by

Required equations

Iω0=(I+mr2) ω1I\omega_0 = (I + mr^2)\,\omega_1

ω1=II+mr2 ω0<ω0\omega_1 = \frac{I}{I + mr^2}\,\omega_0 < \omega_0

Ldisc=Iω1<Iω0L_{disc} = I\omega_1 < I\omega_0

Reasoning and calculation

The flat axis is time tt.

The up axis is the size of LL and ω\omega, for the disc only.

Before the spider (t<0t < 0): the disc spins alone.

Nothing outside twists it.

So L0=Iω0L_0 = I\omega_0 and ω0\omega_0 stay the same. Two flat lines.

At t=0t = 0 the spider lands on the rim.

Very quickly it starts to turn with the disc.

To turn, the spider needs angular momentum.

It gets it from the disc. So the disc's LL goes down.

The disc's II does not change. So its ω\omega goes down too.

After that (t>0t > 0) nothing outside twists it. So both stay at their new, lower values.

0.8 ω00.8\,\omega_0

ω1=I1.25 I ω0\omega_1 = \frac{I}{1.25\,I}\,\omega_0

0.8 L00.8\,L_0

L1=I×0.8 ω0L_1 = I \times 0.8\,\omega_0

So both graphs step down at t=0t = 0, by the same ratio II+mr2\dfrac{I}{I + mr^2}.

Then both stay flat.

They never reach zero.

Reading the options

Only figure (3) shows both dropping at t=0t = 0 and then staying flat.

Why the other options fail

This option says: graph (1): the disc's LL stays the same, only ω\omega drops.

But the disc gives some LL to the spider. So its LL must drop too.

So it is wrong.

This option says: graph (2): ω\omega goes up.

But the disc slows down when the spider lands. ω\omega cannot go up.

This option says: graph (4): LL drops, but ω\omega stays the same.

But L=IωL = I\omega, and the disc's II does not change. If LL drops, ω\omega must drop too.

This option says: graph (5): nothing changes.

But the disc must give the spider some angular momentum. So something must drop.

Conclusion

At t=0t = 0 the disc's LL and ω\omega both drop by the same ratio.

Then they stay the same.

The answer is figure (3).

Saying "angular momentum stays the same" for the disc alone.

It stays the same for disc + spider together.

The question asks about the disc only. That goes down.

Explore

The disc spins at a steady angular speed, with no friction.

At t=0t = 0 the spider lands on the rim and starts to turn with the disc.

The angular momentum the spider needs comes from the disc, so the disc’s LL falls.

The disc’s II does not change, so its ω\omega falls too, and then both stay constant: graph (3).

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