Skip to main content

Unit 6

10–15% of exam

Energy and Momentum of Rotating Systems

This unit brings energy and momentum to spinning objects. A rotating object has rotational kinetic energy, torques do work on it, and its angular momentum changes only when an outside torque acts. You'll use these ideas to analyze rolling objects and satellites in orbit.

Study this unit

Flashcards (30)Practice questions (59)Physics C: Mechanics must-know sheet

Free-response questions on this unit

Write your own answer, then score it with the rubric or with AI.

Big ideas

  • Spinning objects store kinetic energy too
  • A torque acting through an angle does work
  • With no net external torque, angular momentum is conserved
  • Rolling objects have both translational and rotational kinetic energy
  • Orbits follow conservation of energy and angular momentum

Full unit reviews

Longer videos that cover the whole unit. Good for a first pass or a final review.

  • AP Physics C Exam Review (2025): Unit 6 Rotational Energy and Momentum

    Allen Tsao The STEM CoachWatch on YouTube (opens in a new tab)

  • AP Physics C: Mechanics | Unit 6 Review | Energy & Momentum of Rotating Systems

    Prepworks EducationWatch on YouTube (opens in a new tab)

  • AP Physics C: Rotational Dynamics Review - 2 of 2 (Mechanics)

    Flipping PhysicsWatch on YouTube (opens in a new tab)

  • AP Physics 1 - Unit 6 Review - Energy and Momentum of Rotating Systems - Exam Prep

    Flipping PhysicsWatch on YouTube (opens in a new tab)

A rotating object has rotational kinetic energy K=12Iω2K = \frac{1}{2}I\omega^2, even when its center of mass isn't moving, because every piece of it is moving. If an object both moves and spins, its total kinetic energy is its translational kinetic energy plus its rotational kinetic energy about the center of mass.

Key terms

  • rotational kinetic energy
  • rotational inertia
  • angular velocity
  • translational kinetic energy
  • total kinetic energy
  • Topic 6.1 - Rotational Kinetic Energy

    Lessons With LondotWatch on YouTube (opens in a new tab)

  • Rotational kinetic energy of rigid systems | AP Physics | Khan Academy

    Khan AcademyWatch on YouTube (opens in a new tab)

  • Rotational Kinetic Energy Made Easy (with Examples) | AP Physics 1 - Unit 6 Lesson 1

    Allen Tsao The STEM CoachWatch on YouTube (opens in a new tab)

  • Moment of Inertia Introduction and Rotational Kinetic Energy Derivation

    Flipping PhysicsWatch on YouTube (opens in a new tab)

  • 37.1 Kinetic Energy of Translation and Rotation

    MIT OpenCourseWareWatch on YouTube (opens in a new tab)

  • Rotational Kinetic Energy and Moment of Inertia Examples & Physics Problems

    The Organic Chemistry TutorWatch on YouTube (opens in a new tab)

Read the review notes: 6.1 Rotational Kinetic Energy

A few quick questions on this topic, with the answers explained.

A torque that acts while an object turns through an angle does work on it: W=∫τ dθW = \int \tau\,d\theta, or W=τΔθW = \tau\Delta\theta for a constant torque. This work is the area under a graph of torque versus angular position. The net work done by all the torques equals the change in the object's rotational kinetic energy.

Key terms

  • work done by a torque
  • angular displacement
  • work–energy theorem
  • torque–angle graph
  • rotational kinetic energy
  • Topic 6.2 - Torque and Work

    Lessons With LondotWatch on YouTube (opens in a new tab)

  • Rotational Form of Work Simplified | AP Physics 1 - Unit 6 Lesson 3

    Allen Tsao The STEM CoachWatch on YouTube (opens in a new tab)

  • Torque Does Work!!! Awesome!!! | Doc Physics

    Doc SchusterWatch on YouTube (opens in a new tab)

  • Work Done By a Constant Torque - Power & Moment of Inertia - Rotational Motion Physics Problems

    The Organic Chemistry TutorWatch on YouTube (opens in a new tab)

Read the review notes: 6.2 Torque and Work

A few quick questions on this topic, with the answers explained.

Angular momentum is the rotational version of momentum: L=IωL = I\omega for a rigid object and L⃗=r⃗×p⃗\vec{L} = \vec{r} \times \vec{p} for a particle, which has angular momentum about a point even when it moves in a straight line. A net torque changes it, τnet=dLdt\tau_{\text{net}} = \frac{dL}{dt}, and the angular impulse ∫τ dt\int \tau\,dt (the area under a torque–time graph) equals ΔL\Delta L.

Key terms

  • angular momentum
  • angular impulse
  • angular impulse–momentum theorem
  • point particle
  • torque–time graph
  • Topic 6.3 - Angular Momentum and Angular Impulse

    Lessons With LondotWatch on YouTube (opens in a new tab)

  • Angular momentum of rigid systems (with calculus) | AP Physics | Khan Academy

    Khan AcademyWatch on YouTube (opens in a new tab)

  • Angular Impulse & Momentum Made EASY | AP Physics 1 - Unit 6 Lesson 4

    Allen Tsao The STEM CoachWatch on YouTube (opens in a new tab)

  • Angular Momentum of Particles Introduction

    Flipping PhysicsWatch on YouTube (opens in a new tab)

  • AP Physics C - Angular Momentum

    Dan Fullerton (APlusPhysics)Watch on YouTube (opens in a new tab)

  • 34.3 Angular Impulse

    MIT OpenCourseWareWatch on YouTube (opens in a new tab)

Read the review notes: 6.3 Angular Momentum and Angular Impulse

A few quick questions on this topic, with the answers explained.

If the net external torque on a system is zero, its total angular momentum stays constant. A spinning skater who pulls in their arms lowers their rotational inertia, so their angular velocity goes up, and when a lump of clay sticks to a pivoted rod, the angular momentum about the pivot is the same before and after.

Key terms

  • conservation of angular momentum
  • net external torque
  • angular impulse
  • nonrigid system
  • Topic 6.4 - Conservation of Angular Momentum

    Lessons With LondotWatch on YouTube (opens in a new tab)

  • Conservation of angular momentum | AP Physics | Khan Academy

    Khan AcademyWatch on YouTube (opens in a new tab)

  • Conservation of Angular Momentum Introduction and Demonstrations

    Flipping PhysicsWatch on YouTube (opens in a new tab)

  • Conservation of Angular Momentum for Collisions | AP Physics 1 - Unit 6 Lesson 6

    Allen Tsao The STEM CoachWatch on YouTube (opens in a new tab)

  • AP Physics C - Conservation of Angular Momentum

    Dan Fullerton (APlusPhysics)Watch on YouTube (opens in a new tab)

  • Dart with Thin Rod Collision - Conservation of Angular Momentum Demonstration and Problem

    Flipping PhysicsWatch on YouTube (opens in a new tab)

Read the review notes: 6.4 Conservation of Angular Momentum

A few quick questions on this topic, with the answers explained.

An object rolling without slipping has vcm=rωv_{\text{cm}} = r\omega and acm=rαa_{\text{cm}} = r\alpha. Its kinetic energy is split between translation and rotation, which is why a hoop rolls down a ramp more slowly than a solid disk. Static friction helps it roll but does no work on it. If the object slips, kinetic friction takes mechanical energy out, and vcm=rωv_{\text{cm}} = r\omega no longer holds.

Key terms

  • rolling without slipping
  • rolling with slipping
  • static friction
  • kinetic friction
  • translational kinetic energy
  • rotational kinetic energy
  • Topic 6.5 - Rolling

    Lessons With LondotWatch on YouTube (opens in a new tab)

  • Advanced Rolling Motion Explained | AP Physics C - Unit 5 - Lesson 8C

    Allen Tsao The STEM CoachWatch on YouTube (opens in a new tab)

  • Rolling Without Slipping Introduction and Demonstrations

    Flipping PhysicsWatch on YouTube (opens in a new tab)

  • Rolling without slipping problems | Physics | Khan Academy

    Khan Academy PhysicsWatch on YouTube (opens in a new tab)

  • 35.4 Rolling Without Slipping Slipping and Skidding

    MIT OpenCourseWareWatch on YouTube (opens in a new tab)

  • Bowling Ball Sliding Problem

    Physics NinjaWatch on YouTube (opens in a new tab)

Read the review notes: 6.5 Rolling

A few quick questions on this topic, with the answers explained.

For a satellite orbiting a much more massive object, the gravitational potential energy is U=−GMmrU = -\frac{GMm}{r}, which is zero when they're infinitely far apart. In a circular orbit the speed, kinetic energy and potential energy all stay constant. In an elliptical orbit only the total energy and angular momentum stay constant, so the satellite speeds up as it gets closer. Escape velocity, vesc=2GMrv_{\text{esc}} = \sqrt{\frac{2GM}{r}}, is the launch speed that makes the total mechanical energy zero.

Key terms

  • gravitational potential energy
  • circular orbit
  • elliptical orbit
  • escape velocity
  • total mechanical energy
  • angular momentum
  • Topic 6.6 - Motion of Orbiting Satellites

    Lessons With LondotWatch on YouTube (opens in a new tab)

  • Energy of satellite systems | AP Physics | Khan Academy

    Khan AcademyWatch on YouTube (opens in a new tab)

  • Mechanical Energy of a Satellite in Circular Orbit

    Flipping PhysicsWatch on YouTube (opens in a new tab)

  • Angular momentum of satellites | AP Physics | Khan Academy

    Khan AcademyWatch on YouTube (opens in a new tab)

  • AP Physics C - Orbits

    Dan Fullerton (APlusPhysics)Watch on YouTube (opens in a new tab)

  • Deriving Escape Velocity of Planet Earth

    Flipping PhysicsWatch on YouTube (opens in a new tab)

Read the review notes: 6.6 Motion of Orbiting Satellites

A few quick questions on this topic, with the answers explained.