Rolling
A short lesson with diagrams, a worked example, a problem to try, and a quick check. Then quiz yourself on 5 practice questions.
Rolling without slipping links spin and motion: vcm = Rω and acm = Rα. The contact point is momentarily at rest. A rolling object’s kinetic energy has two parts: ½Mv² + ½Icmω².
1. Forces on a rolling object
2. Shape decides the race
Mass and radius cancel out; only the shape factor I/MR² matters. Objects that store less energy in spin have more left for moving forward.
Static friction does no work on a rolling object, because the contact point doesn’t slide. Mechanical energy is conserved.
3. Example, then try it
A 2.0 kg hoop rolls at 3.0 m/s. Find its kinetic energy.
For a hoop I = MR², so ½Iω² = ½MR²(v/R)² = ½Mv². K = ½Mv² + ½Mv² = Mv² = (2.0)(3.0)² = 18 J, half of it rotational.
A 2.0 kg solid sphere rolls without slipping down a 30° incline. Find its acceleration, the friction force on it, and the minimum μs needed. How fast is it going after dropping 1.4 m? (g = 10 m/s²)
Acceleration: a = g sin θ ÷ (1 + 2/5) = 5.0 ÷ 1.4 ≈ 3.6 m/s².
Friction: torque fR = I(a/R), so f = (2/5)Ma = (0.40)(2.0)(3.57) ≈ 2.9 N, up the slope.
Minimum μs: f/N = 2.9 ÷ (2.0 × 10 × cos 30°) = 2.9 ÷ 17.3 ≈ 0.17.
Speed: v² = 2gh ÷ 1.4 = 28 ÷ 1.4 = 20, so v ≈ 4.5 m/s.
Answer: 3.6 m/s², 2.9 N of friction, μs ≥ 0.17, 4.5 m/s after 1.4 m.
4. Common mistakes
Two solid cylinders of different masses and radii roll without slipping down the same ramp from rest. Which reaches the bottom first?
a = g sin θ / (1 + I/MR²), and I/MR² = ½ for every solid cylinder. Mass and radius cancel, so they tie.
Ready to practice?
5 questions on Rolling, each with a hint and an explanation for every wrong answer.
