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AP® Physics 1: Algebra-Based · Unit 5 · Topic 5.4

Rotational Inertia: Revision Notes (Physics 1 5.4)

One-page recap of rotational inertia for the algebra-based course: I = mr², adding point masses, the centre-of-mass minimum, the parallel axis theorem and hoops versus disks.

Short on time? This page is the recap. For explanations, the graph and worked examples, use the full study guide. This is the algebra-based course: no calculus is needed.

Recap

  • Rotational inertia I measures how hard it is to change a rigid system’s rotation. It is the rotational partner of inertial mass.
  • It depends on the mass and on the distribution of mass relative to the axis. Mass far from the axis counts much more than mass near it.
  • One object has a different I for every axis. Always state the axis.
  • You calculate I for up to five small objects in a flat layout. For rods, disks, hoops and spheres, the value is given.
  • For any family of parallel axes, I is smallest through the centre of mass.
  • Compare a hoop with a solid disk of equal mass and radius: the hoop’s I is larger, because all its mass is at the rim.

Key relationships

Relationship Symbols and units Use it to
I = mr² m in kg, r = perpendicular distance from axis in m; I in kg·m² find I for one small object
I = Σmᵢrᵢ² every rᵢ from the same axis add up a system of small objects
I = I_cm + Md² M = total mass; d = distance between the parallel axes move from the centre-of-mass axis to a parallel one
I_new / I_old = (r_new / r_old)² same mass factor-of-change questions

Assumptions behind the numbers

  • The system is rigid: the masses stay at fixed distances from the axis.
  • “Small” objects are treated as points at a single distance r.
  • Connecting rods or frames described as light add nothing to I.
  • Formulas for extended objects (such as ½MR² for a disk) are given, and apply only to the axis stated with them.

Mistakes to avoid

  1. Not squaring r. I = mr², not mr.
  2. Measuring r from the wrong point. Use the perpendicular distance from the stated axis.
  3. Assuming one I per object. Change the axis and I changes.
  4. Using part of the mass in Md². M is the total mass of the system.
  5. Starting the parallel axis theorem from the wrong axis. It must start from I_cm.
  6. Thinking more material always means more I. A hoop beats a disk of the same mass and radius.
  7. Putting the minimum at the geometric centre when the masses are unequal. It is at the centre of mass.

Quick self-check

  1. A 0.30 kg bead is 0.20 m from an axis. Find I. (0.012 kg·m²)
  2. A 2.0 kg object has I_cm = 0.050 kg·m². Find I about a parallel axis 0.10 m away. (0.070 kg·m²)
  3. A small mass is moved from 0.15 m to 0.30 m from the axis. By what factor does its I change? (4 times as large)

Next: practice questions.

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