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AP® Physics C: Mechanics · Unit 2 · Topic 2.10

Circular Motion: Revision Notes (Physics C: Mechanics 2.10)

One-page recap of circular motion: centripetal and tangential acceleration, period and frequency, loops, banked curves with friction, conical pendulums and Kepler's third law.

Short on time? This page is the recap. For the derivations, figures and three worked examples, use the full study guide.

Recap

  • On a circle the velocity’s direction changes, so the object accelerates even at constant speed.
  • Differentiating r(t) = r cos(ωt) î + r sin(ωt) ĵ twice gives a = −ω²r: size v²/r, pointing to the centre.
  • If the speed changes, add tangential acceleration a_t = dv/dt, perpendicular to a_c.
  • Take + toward the centre for the radial equation. “Centripetal force” is the inward net force, never an extra arrow.

Key relationships

Relationship Condition or meaning
a_c = v²/r = 4π²r/T² toward the centre; v²/r holds on any circular path, the T form only at constant speed
a_t = dv/dt = d²s/dt² along the velocity; zero for uniform circular motion
|a| = √(a_c² + a_t²) net acceleration
T = 1/f; T = 2πr/v uniform circular motion
ΣF toward centre = mv²/r Newton’s second law along the radius
v_min = √(gr) top of a vertical loop, when N (or tension) is zero
v² = rg tan θ banked curve needing no friction
v_max² = rg(sin θ + μ_s cos θ)/(cos θ − μ_s sin θ) banked curve, friction down the slope
tan θ = v²/(rg); T = 2π√(L cos θ/g) conical pendulum
T² = (4π²/GM) r³ circular orbit, gravity the only force

For v_min on a banked curve, change the sign of every μ_s term. If tan θ ≤ μ_s there is no minimum.

Assumptions

  • Inertial reference frame; objects treated as points.
  • g = 9.8 m/s² near Earth’s surface; orbit radius measured from the planet’s centre.
  • Kepler’s first and second laws are not needed: orbits here are circles.

Mistakes to avoid

  1. Drawing a “centripetal force” arrow on a free-body diagram.
  2. Assuming the net force points to the centre when the speed is changing.
  3. Fixing friction’s direction on a banked curve before checking the speed.
  4. Using altitude instead of orbit radius.
  5. Normal force up at the top of a loop (inside the track, it points down).
  6. Using frequency in place of 2πf when finding speed: v = 2πrf.

Quick self-check

  1. A car goes round a bend of radius 16 m at 8.0 m/s. Find a_c. (64 ÷ 16 = 4.0 m/s²)
  2. A ball on a string moves in a circle of radius 0.50 m at 2.0 Hz. Find T, v and a_c. (T = 0.50 s; v = 2π × 0.50 × 2.0 ≈ 6.3 m/s; a_c ≈ 79 m/s²)
  3. What is the minimum speed at the top of a loop of radius 0.90 m? (√(9.8 × 0.90) ≈ 3.0 m/s)

Next: practice questions.

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