Translational Kinetic Energy
Define K = (1/2)mv^2, recognize it as a scalar, and explain why its value depends on the observer's reference frame.
Unit 3 builds the energy toolkit: kinetic energy, work as a line integral, potential energy stored by conservative forces, conservation of mechanical energy, and power as the rate of energy transfer. These ideas give you a second method for solving dynamics problems alongside Newton's second law from Unit 2.
Fiveable's AP Physics C: Mechanics Unit 3 review covers 5 topics, with guided practice questions for the unit.
Define K = (1/2)mv^2, recognize it as a scalar, and explain why its value depends on the observer's reference frame.
Calculate work using W = Fd cos(theta) for constant forces and W = integral F dot dr for variable forces. Distinguish conservative from nonconservative forces and apply the work-energy theorem.
Derive potential energy functions from conservative forces using delta U = -integral F dot dr, extract force from F_x = -dU/dx, and identify equilibrium from U(x) graphs.
Apply E = K + U for conservative systems and W_nc = delta E when nonconservative forces act. Choose system boundaries to set up energy equations correctly.
Calculate average power with P_avg = W / delta t and instantaneous power with P_inst = dW/dt or P = Fv cos(theta). Convert between watts and other energy-rate units.
Try AP-style questions on unit 3, then use the review notes below for anything you miss.
A timed, AP-style test built only from unit 3 questions — multiple choice plus free response, scored with AI feedback. Use the standard format or build your own.
Translational kinetic energy is the energy an object has due to its translational motion. It is always a scalar and always non-negative. Because kinetic energy depends on v^2, doubling speed quadruples K. The value of K depends on the observer's reference frame, so two inertial observers can legitimately measure different values for the same object.
A 2 kg object moves at 3 m/s in one frame and 5 m/s in another. Calculate K in each frame and confirm that both values are physically valid.
| Quantity | Depends on mass? | Depends on speed? | Scalar or vector? |
|---|---|---|---|
| Kinetic energy K | Yes, linearly | Yes, quadratically | Scalar |
| Momentum p | Yes, linearly | Yes, linearly | Vector |
Work is the energy transferred into or out of a system by a force acting over a displacement. For a constant force, W = Fd cos(theta), where theta is the angle between force and displacement. For a variable force, W = integral from a to b of F(r) dot dr. The area under a graph of the force component parallel to displacement versus displacement equals the work done. Conservative forces do path-independent work; nonconservative forces like kinetic friction do path-dependent work.
A spring with k = 200 N/m is compressed 0.10 m from equilibrium. Use the line integral to find the work done by the spring as it returns to equilibrium.
| Force type | Path dependent? | Associated potential energy? | Example |
|---|---|---|---|
| Conservative | No | Yes | Gravity, spring |
| Nonconservative | Yes | No | Kinetic friction, air resistance |
Potential energy is stored energy associated with the configuration of a system whose objects interact through conservative forces. It is a scalar tied to position. The zero reference point is chosen by the analyst to simplify calculation; only changes in potential energy are physically meaningful. The key calculus relationship is delta U = -integral of F_cf dot dr, or equivalently F_x = -dU/dx in one dimension. A U(x) graph encodes both the potential energy and the force at every position.
Given U(x) = 3x^2 - 12x (in joules, x in meters), find the equilibrium position and determine whether it is stable or unstable.
| System | Potential energy formula | Zero reference convention |
|---|---|---|
| Object near Earth's surface | U_g = mgy | Chosen height y = 0 |
| Spring-mass system | U_s = (1/2)kx^2 | Natural length x = 0 |
| Two point masses (gravitation) | U = -Gm1m2/r | Zero at r = infinity |
Mechanical energy is E = K + U. When only conservative forces act within a chosen system and no work is done on the system from outside, E is constant: K_i + U_i = K_f + U_f. When nonconservative forces act, the work they do equals the change in total mechanical energy: W_nc = delta E = delta K + delta U. Choosing the system boundary carefully determines which forces are internal and which do work across the boundary.
A 1 kg block slides down a 2 m ramp inclined at 30 degrees with a coefficient of kinetic friction of 0.2. Use energy methods to find the speed at the bottom.
| Scenario | Mechanical energy conserved? | Equation to use |
|---|---|---|
| Only conservative forces | Yes | K_i + U_i = K_f + U_f |
| Friction or drag present | No | K_i + U_i + W_nc = K_f + U_f |
| External force does work | No | W_ext = delta K + delta U |
Power is the rate at which energy is transferred or converted. Average power is P_avg = delta E / delta t or equivalently W / delta t. Instantaneous power is P_inst = dW/dt. When a constant force acts on an object moving at velocity v, instantaneous power simplifies to P_inst = F_parallel * v = Fv cos(theta). The SI unit of power is the watt (1 W = 1 J/s).
A motor exerts a constant 500 N force on a cart moving at 4 m/s at an angle of 30 degrees between force and velocity. Calculate the instantaneous power delivered.
| Formula | When to use | Variables needed |
|---|---|---|
| P_avg = W / delta t | Total work over a time interval is known | W, delta t |
| P_avg = delta E / delta t | Energy change over a time interval is known | delta E, delta t |
| P_inst = dW/dt | Work is a function of time | W(t) expression |
| P_inst = Fv cos(theta) | Constant force, known velocity | F, v, theta |
| Term | Definition |
|---|---|
| scalar | A physical quantity described by magnitude only, without direction. Both kinetic energy and work are scalars. |
Miss rates come from Fiveable multiple-choice practice.
Work is a scalar. The dot product F dot dr produces a signed number, not a vector. Students sometimes try to add work values as vectors, which gives wrong answers.
The conservative force equals the negative derivative of potential energy. Dropping the negative sign reverses the direction of the force and leads to incorrect equilibrium analysis.
K_i + U_i = K_f + U_f only holds when all forces doing work are conservative. If kinetic friction or drag acts, you must include W_nc = delta E or the answer will be too large.
P_avg = W / delta t gives the average rate over an interval. P_inst = Fv cos(theta) gives the rate at one instant. Using the average formula when instantaneous power is asked, or vice versa, produces incorrect results.
The zero reference for U is a free choice, but it must stay consistent throughout a single problem. Switching the reference mid-calculation changes delta U and breaks the energy equation.
AP Physics C: Mechanics free-response questions frequently ask you to derive a symbolic expression for work, potential energy, or power using integration or differentiation. You should be comfortable setting up the line integral W = integral F dot dr for a given force function and applying F_x = -dU/dx to extract force from a potential energy expression.
Exam questions often ask you to explain whether mechanical energy is conserved in a given scenario and to justify your answer. You need to identify which forces act, classify them as conservative or nonconservative, and state how that classification determines whether E = K + U is constant or whether W_nc = delta E applies.
Questions may present a U(x) graph and ask you to identify equilibrium positions, determine the direction of force at a given point, or sketch the corresponding F(x) graph. You may also be asked to find work as the area under an F vs displacement curve or to read instantaneous power from a slope on an energy versus time graph.
Open the individual guides for Unit 3 when you want a closer review of one topic.
Use AP-style practice after you review the notes so you can check what you understand.
Practice free-response reasoning and compare your answer with scoring guidance.
Watch past review streams filtered to Unit 3 when you want a video walkthrough.
Open the Fiveable one-page unit review, then explore visual cheatsheets for a quick refresher.
Estimate your broader AP score goal after you review the course and exam format.

Print the unit cheatsheets ($3) for Unit 3. Yours to keep, no subscription needed.
get printablesThe AP Classroom Unit 3 progress check includes both MCQ and FRQ parts drawn from all five Unit 3 topics: Translational Kinetic Energy, Work, Potential Energy, Conservation of Energy, and Power. The MCQ section tests conceptual reasoning and calculation, while the FRQ part asks you to apply the work-energy theorem and conservation of energy to multi-part scenarios. Practice with matched questions at AP Physics C: Mechanics Unit 3.
Unit 3 FRQs most often come from Conservation of Energy (3.4) and Work (3.2), asking you to set up energy equations, justify sign conventions, and interpret graphs of force vs. displacement. Practice by writing out full solutions that include a clear energy diagram, labeled variables, and a written justification, not just a numerical answer. Find Unit 3 FRQ practice at AP Physics C: Mechanics Unit 3.
The best place to find AP Physics C: Mechanics Unit 3 practice questions, including multiple-choice and practice test sets, is AP Physics C: Mechanics Unit 3. That page organizes MCQ and FRQ practice by topic, covering Translational Kinetic Energy, Work, Potential Energy, Conservation of Energy, and Power so you can target whichever topic needs the most work.
Start with Work (3.2) and the work-energy theorem before moving to Potential Energy (3.3) and Conservation of Energy (3.4), since those topics build directly on each other. Sketch energy diagrams for every problem, practice setting up integrals for variable forces, and check your sign conventions carefully. Finish by connecting Power (3.5) to the rate of energy transfer in real scenarios. Use the topic-by-topic resources at AP Physics C: Mechanics Unit 3 to track your progress.