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AP® Physics C: Mechanics · Unit 3 · Topic 3.3

Potential Energy: Revision Notes (Physics C: Mechanics 3.3)

One-page calculus recap of potential energy: ΔU = −∫F·dr, F_x = −dU/dx, stable and unstable equilibrium, spring and gravitational potential energy, and adding pair energies.

Short on time? This page is the recap for the calculus-based course (separate from Physics 1). For derivations, the U(x) graph and worked examples, use the full study guide.

Recap

  • Potential energy is a scalar stored in the arrangement of a system of two or more objects.
  • It exists only for conservative interactions: work independent of path, zero around a closed loop. Friction has no potential energy.
  • You choose where U = 0. Only changes in U are physical.
  • The conservative force points towards lower U.
  • For three or more objects, add the energy of every pair once.

Key relationships

Relationship Units Notes
ΔU = −W_c = −∫F_c · dr J defines U from a conservative force
F_x = −dU/dx N minus the slope of the U(x) graph
dU/dx = 0 — equilibrium position
d²U/dx² > 0 / < 0 — stable (minimum) / unstable (maximum)
U_s = ½k(Δx)² J ideal spring, U = 0 at relaxed length
U_g = −Gm₁m₂/r J spheres, U = 0 at infinite separation
ΔU_g ≈ mgΔy J near a surface, Δy much smaller than the radius
U = U₁₂ + U₁₃ + U₂₃ + … J systems of three or more objects

Assumptions behind the numbers

  • One-dimensional motion along a stated axis unless told otherwise.
  • Ideal spring: massless, force proportional to deformation.
  • Spheres act as point masses at their centres. g = 9.8 m/s²; G = 6.67 × 10⁻¹¹ N·m²/kg².

Mistakes to avoid

  1. “An object has potential energy.” A system does.
  2. Losing the minus sign in ΔU = −W_c or F_x = −dU/dx.
  3. Equilibrium where U = 0. Equilibrium is where the slope is zero.
  4. Stable at a maximum. A maximum pushes the object away.
  5. mgΔy for large heights. Use −Gm₁m₂/r.
  6. ½k(Δx)² for a nonideal spring. Integrate the actual force.
  7. Counting a pair twice in a many-body system.

Quick self-check

  1. U(x) = (4.0 J/m²)x². What is F_x at x = 0.50 m? (−dU/dx = −8.0x = −4.0 N)
  2. A spring has k = 200 N/m. How much does U_s rise when the stretch goes from 0.050 m to 0.10 m? (½ × 200 × (0.010 − 0.0025) = 0.75 J)
  3. U(x) has a local maximum at x = 3.0 m. Is that equilibrium stable? (No. A small push gives a force away from 3.0 m: unstable.)

Next: practice questions.

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