Rotational motion and gravitation

Physics · Mathematical methods and mechanics. The idea in plain words, the rules to remember, the mistake to avoid and a worked example, written and checked by Mega Lecture.

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The idea

Rotation copies linear motion. Torque takes the place of force, moment of inertia I takes the place of mass and angular momentum L = Iω takes the place of momentum. I depends on how far the mass lies from the axis, so the same body has different values of I about different axes. If no external torque acts, L stays constant.

Gravitation is an inverse-square attraction between masses, with distances measured between centres. In a circular orbit gravity supplies the centripetal force, which fixes the orbital speed and period at each radius.

Kepler's laws follow from this: orbits are ellipses, the line to the Sun sweeps equal areas in equal times, and T2 ∝ r3.

Rules to remember

Common mistake

Measuring distance from the surface instead of from the centre. At a height equal to the Earth's radius, r = 2R, so g falls to one quarter, not one half.

Worked example

A turntable is a uniform disc of mass 6 kg and radius 0.5 m, spinning freely at 4 rad s−1. A 1 kg lump of clay is dropped onto its rim and sticks. Find the new angular speed.

  1. Disc: I1 = ½ × 6 × 0.52 = 0.75 kg m2.
  2. With the clay: I2 = 0.75 + 1 × 0.52 = 1.0 kg m2.
  3. No external torque, so I1ω1 = I2ω2: ω2 = 0.75 × 4 ÷ 1.0 = 3 rad s−1.
  4. Kinetic energy falls from ½ × 0.75 × 42 = 6 J to ½ × 1.0 × 32 = 4.5 J, because the clay sticks.

Answer: 3 rad s−1.

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