Rotational Inertia
Topic 5.3 named the rotational input, torque. Topic 5.4 names the rotational resistance: rotational inertia, the rotational analog of mass. Force changes velocity, and a body's mass sets how much velocity-change a given force buys. Torque changes angular velocity, and a body's rotational inertia $I$ sets how much.
The catch: where mass is a property of an object alone, $I$ is a property of an object about an axis. The same body has different $I$ values about different axes, and the way mass is distributed matters at least as much as the total mass. The headline definition for a system of point masses, $I = \sum_i m_i r_i^2$, makes both factors plain: mass enters linearly, distance from the axis enters squared.
Two common traps. First, deciding which body has more $I$ by looking at one factor in isolation: heavier wins ignoring the geometry, or more spread out wins ignoring the mass. The formula has both factors and neither one decides on its own. Second, treating $I$ as a property of the body alone. The same rod about its center versus about one end has rotational inertias that differ by a factor of four. Specify the axis before you quote a rotational inertia.
The work
3 ways in · any order
Lesson
Rotational Inertia
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Build $I$ from scratch: the definition $I = \sum m_i r_i^2$, the five standard shape formulas from the AP equation sheet, the axis-dependence of $I$, and the parallel-axis theorem. Closes with a ten-scenario applet that targets the mass-and-distribution trap and the axis-independence trap.
Diagnostic
10-item topic check
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Ten items, mixed symbolic, factor-of-change, quantitative, and conceptual. Each wrong-answer chip is tagged with a specific misconception code; whichever traps fire seed your targeted-practice queue. Plan on about 15 minutes.
Targeted Practice
Drill a single misconception
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Pick one of the failure modes you've missed and grind it on its own. The round is adaptive: two correct in a row clears the misconception and you move on.