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Unit 3

15–25% of exam

Work, Energy, and Power

Energy gives you a second way to solve motion problems, often faster than using forces. Work is how a force moves energy into or out of a system, and in this course you find it with an integral, W=∫F⃗⋅dr⃗W = \int\vec{F}\cdot d\vec{r}. You'll link conservative forces to potential energy, use conservation of energy to connect the start and end of a process, and describe how fast energy moves as power.

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Flashcards (30)Practice questions (54)Physics C: Mechanics must-know sheet

Free-response questions on this unit

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Big ideas

  • Work transfers energy into or out of a system
  • Net work equals the change in kinetic energy
  • A conservative force points toward lower potential energy: Fx=−dUdxF_x = -\frac{dU}{dx}
  • Energy is always conserved; your choice of system decides whether it stays constant
  • Power is the rate of energy transfer

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 3 Work and Energy

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

  • AP Physics C: Work, Energy, and Power Review (Mechanics)

    Flipping PhysicsWatch on YouTube (opens in a new tab)

  • AP Physics C: Mechanics | Unit 3 Review | Work, Energy, and Power (EVERYTHING YOU NEED TO KNOW!!)

    Prepworks EducationWatch on YouTube (opens in a new tab)

  • AP Physics C Mechanics Unit 3 Energy Review

    Physics and Math with Dr. D'AntuonoWatch on YouTube (opens in a new tab)

Translational kinetic energy, K=12mv2K = \frac{1}{2}mv^2, is the energy an object has because it is moving. It's a scalar, so direction doesn't matter and it is never negative. Observers in different reference frames measure different speeds, so they can measure different kinetic energies for the same object.

Key terms

  • kinetic energy
  • scalar
  • speed
  • reference frame
  • joule
Read the review notes: 3.1 Translational Kinetic Energy

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

3.2

Work

Work is energy transferred into or out of a system by a force acting over a displacement: W=∫abF⃗⋅dr⃗W = \int_a^b\vec{F}\cdot d\vec{r}. It equals the area under a graph of the force component along the motion versus position. Only that parallel component does work, so work can be positive, negative or zero. By the work–energy theorem, the net work on an object equals its change in kinetic energy. Work done by a conservative force like gravity doesn't depend on the path taken, but work done by friction does.

Key terms

  • work
  • dot product
  • work–energy theorem
  • conservative force
  • nonconservative force
  • force–position graph
  • Work done by forces (part 1) | AP Physics | Khan Academy

    Khan AcademyWatch on YouTube (opens in a new tab)

  • Topic 3.2 - Work

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

  • Deriving the Work-Energy Theorem using Calculus

    Flipping PhysicsWatch on YouTube (opens in a new tab)

  • AP Physics C - Work

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

  • AP Physics C Mechanics - Unit 3 - Lesson 1C - Work (Integral Form)

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

  • 20.3 Work by a Non-Constant Force

    MIT OpenCourseWareWatch on YouTube (opens in a new tab)

Read the review notes: 3.2 Work

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

Potential energy belongs to a system of objects that interact through conservative forces, and it depends on their positions: ΔU=−∫F⃗⋅dr⃗\Delta U = -\int\vec{F}\cdot d\vec{r} and Fx=−dUdxF_x = -\frac{dU}{dx}. On a U(x) graph, minimums are stable equilibrium points and maximums are unstable ones. Key cases are a spring, Us=12k(Δx)2U_s = \frac{1}{2}k(\Delta x)^2, gravity near Earth, ΔUg=mgΔy\Delta U_g = mg\Delta y, and gravity between spherical bodies, UG=−Gm1m2rU_G = -\frac{Gm_1m_2}{r}.

Key terms

  • potential energy
  • conservative force
  • potential energy graph
  • stable equilibrium
  • unstable equilibrium
  • zero of potential energy
  • Potential energy and conservative forces (part 1) | AP Physics | Khan Academy

    Khan AcademyWatch on YouTube (opens in a new tab)

  • Topic 3.3 - Potential Energy

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

  • Conservative Force and Potential Energy

    Flipping PhysicsWatch on YouTube (opens in a new tab)

  • AP Physics C - Potential Energy and Conservative Forces

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

  • AP Physics C Mechanics - Unit 3 - Lesson 11C - Graphs of Potential Energy

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

  • 25.1 Force is the Derivative of Potential

    MIT OpenCourseWareWatch on YouTube (opens in a new tab)

Read the review notes: 3.3 Potential Energy

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

Mechanical energy is the sum of a system's kinetic and potential energies. If no external work is done on the system and nothing like friction acts inside it, its mechanical energy stays constant; otherwise energy is transferred between the system and its surroundings or turned into thermal energy and sound. Choosing the system carefully decides which energies you track and whether the total stays the same.

Key terms

  • mechanical energy
  • conservation of energy
  • system
  • external work
  • energy dissipation
  • Conservation of energy (part 1) | AP Physics | Khan Academy

    Khan AcademyWatch on YouTube (opens in a new tab)

  • Topic 3.4 - Conservation of Energy

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

  • Introduction to Conservation of Mechanical Energy with Demonstrations

    Flipping PhysicsWatch on YouTube (opens in a new tab)

  • AP Physics C - Conservation of Energy

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

  • 24.1 Mechanical Energy and Energy Conservation

    MIT OpenCourseWareWatch on YouTube (opens in a new tab)

  • Energy Systems Clarified

    Flipping PhysicsWatch on YouTube (opens in a new tab)

Read the review notes: 3.4 Conservation of Energy

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

Power is how fast energy is transferred or changed from one form to another: average power is Pavg=ΔEΔtP_{avg} = \frac{\Delta E}{\Delta t} and instantaneous power is P=dWdtP = \frac{dW}{dt}. For a force on a moving object, P=F⃗⋅v⃗P = \vec{F}\cdot\vec{v}, so only the force component along the velocity delivers power. Power is measured in watts, or joules per second.

Key terms

  • power
  • average power
  • instantaneous power
  • watt
  • rate of energy transfer
Read the review notes: 3.5 Power

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