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AP® Physics C: Mechanics · Unit 2 · Topic 2.6

Gravitational Force: Revision Notes (Physics C: Mechanics 2.6)

One-page recap of gravitation for the calculus-based course: the universal law, field and weight, constant g, apparent weight, the two kinds of mass, and spheres and shells.

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

Recap

  • Gravity is attractive, acts along the line of centers, and can be taken to act at each system’s center of mass.
  • The two forces in a pair are equal in size; the accelerations are not.
  • The field is force per unit mass. With gravity as the only force, a = g.
  • Weight = mg. Treat g as constant when r hardly changes (near Earth’s surface, g ≈ 9.8 N/kg).
  • Apparent weight is the normal force. Weightless means N = 0: no forces at all, or gravity alone.
  • Equivalence principle: inside a closed cabin you cannot tell a gravitational field from an acceleration of the cabin.
  • Inertial mass (resists change in motion) and gravitational mass (takes part in attraction) are found by experiment to be equal.

Key relationships

Relationship Units Notes
F_g = G m₁m₂ / r² N G = 6.67 × 10⁻¹¹ N·m²/kg²; r between centers
g = F_g/m = GM/r² N/kg = m/s² points toward M
W = mg N near a planet’s surface
N = m(g + a_y) N +y upward; apparent weight
g_surface = (4/3)πGρR N/kg uniform planet; same ρ, double R → double g
Thin shell: F = 0 inside; GMm/r² outside N shell theorem, used without proof
Uniform sphere inside: M_partial = Mr³/R³, F = (GMm/R³)r = kr N toward center: F = −kr

Assumptions behind the numbers

  • Spheres are uniform (or made of uniform shells); other bodies’ pulls are ignored unless stated.
  • Constant g only over heights that are small compared with the planet’s radius (g falls 1% by about 32 km above Earth).
  • Air resistance ignored for “free fall”.

Mistakes to avoid

  1. Using the altitude as r. Add the planet’s radius.
  2. Forgetting to square r, or squaring the mass instead.
  3. Saying apparent weight depends on velocity. It depends on acceleration.
  4. Using the whole mass inside a sphere. Only the partial mass within r counts.
  5. Thinking the field inside a shell is zero only at the center. It is zero everywhere inside.
  6. “Weightless means no gravity.” It means nothing pushes back against gravity.

Quick self-check

  1. Two masses move twice as far apart. What happens to F_g? (It becomes ¼ as large.)
  2. g at a planet’s surface is 9.8 N/kg. What is it at r = 2R? (2.45 N/kg)
  3. A 50 kg person in a lift accelerating upward at 2.0 m/s². What does the scale read? (50 × 11.8 = 590 N)

Next: practice questions.

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