AS 91524 · 2024 paper · circular motion of a ball bearing
Question 1(d) Merit to Excellence
Practises Energy methods for rolling and rotating bodies
A solid steel ball bearing is released from different heights on a steel track. It rolls down and travels over a series of bumps and dips, each of radius 35.0 mm. Point X is the bottom of the first dip; Point Y is the top of a bump. As a solid sphere, I = ⅖mr².
| r ball | 7.00 mm |
|---|---|
| m | 11.2 g |
| bump/dip radius | 35.0 mm |
By considering energy changes, calculate the maximum height h above Point Y that the ball can be released from if it is to stay in contact with the track over the bumps (a solid sphere, I = ⅖mr²).
Work it out
Try it on paper first. Stuck? Take one hint at a time.
-
1 To stay on the track at Y, what is the most speed the ball can have there?
From (b), v = √(gr), so v² = gr = 9.81 × 0.0350 = 0.343 35 m² s⁻². -
2 Released from rest a height h above Y, where has its gravitational potential energy gone by the time it gets to Y?
Into kinetic energy of two kinds, because it rolls: mgh = ½mv² + ½Iω². -
3 Put in I = ⅖mr² and ω = v / r. What happens to the ball’s radius?
½Iω² = ½ × ⅖mr² × v² / r² = ⅕mv². So mgh = ½mv² + ⅕mv² = 0.7mv². The ball’s mass and its radius both cancel. -
4 Solve for h.
h = 0.7v² / g = 0.7 × 0.343 35 / 9.81 = 0.0245 m. -
5 Check it with the energies themselves.
With m = 0.0112 kg: mgh = 0.0112 × 9.81 × 0.0245 = 2.692 × 10⁻³ J, which splits into ½mv² = 1.923 × 10⁻³ J and ½Iω² = 0.769 × 10⁻³ J (the ball spins at ω = 0.586 / 0.00700 = 83.7 rad s⁻¹).
What the marker wanted
- Achieved One of: an attempt by conservation of energy (Egp = Ek(lin) + Ek(rot)); one energy right (Ek(lin) = 1.92 × 10⁻³ J or Ek(rot) = 7.69 × 10⁻⁴ J); or the spin at Y, ω = 83.7 rad s⁻¹.
- Merit The right process with one error, such as a slip while simplifying; or two of the three energies right, having tried all three; or h = 7.00 × 10⁻³ m.
- Excellence The right answer, 0.0245 m.
In our words, from NZQA’s 2024 marking schedule.
✕Common mistake
Counting only one kind of kinetic energy. Using the rotational energy alone gives h = 7.00 × 10⁻³ m, which the schedule holds at Merit. The ball both moves along and spins, so it needs ½mv² and ½Iω² at Y.How did it go?
Got it moves it further out. Review brings it back tomorrow.