Rotational Inertia

Noah Martinez
7 min read
Study Guide Overview
This study guide covers rotational inertia, also known as the moment of inertia. It explains the concept, the formula (), and how mass distribution affects it. The guide also covers calculating rotational inertia for rigid systems and off-center rotations using the parallel axis theorem (). Finally, it provides practice questions and exam tips.
#AP Physics 1: Rotational Inertia - The Night Before 🚀
Hey! Let's make sure you're totally ready for the exam tomorrow. We're going to break down rotational inertia, make it super clear, and get you feeling confident. This is your go-to guide for a last-minute review.
#Rotational Inertia: What's the Deal?
Rotational inertia, also known as the moment of inertia, is all about how hard it is to change an object's spin. Think of it as the rotational version of mass. It's not just about how much stuff there is, but where that stuff is located relative to the axis of rotation.
- Key Idea: The farther the mass is from the axis of rotation, the harder it is to start or stop it from spinning. 💡
Memory Aid: Imagine a figure skater. When they pull their arms in, they spin faster (lower rotational inertia). When they extend their arms, they slow down (higher rotational inertia). It's all about how the mass is distributed!
#Rotational Inertia of Rigid Systems
#Resistance to Rotational Changes
- Rotational inertia measures a system's resistance to changes in its rotational motion. 🔄
- It depends on the total mass and its distribution relative to the axis of rotation.
- More mass farther from the axis = greater rotational inertia.
- Example: A figure skater extending arms increases rotational inertia, slowing their spin.
#Equation for Rotational Inertia
- For a single point mass:
- = rotational inertia (kg⋅m²)
- = mass (kg)
- = perpendicular distance from the axis (m)
- For multiple objects: (sum of individual inertias)
- Example: Two masses, 2 kg and 3 kg, are attached to a rod at distances of 0.5 m and 1 m from the axis. The total rotational inertia is:

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