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AP® Physics C: Mechanics · Unit 2 · Topic 2.1

Systems and Center of Mass: Revision Notes (Physics C: Mechanics 2.1)

One-page recap of systems and center of mass: choosing a system, when it is one object, the particle formula, symmetry, and integrals with linear, area and volume mass density.

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

Recap

  • A system is what you put inside a boundary; the rest is the environment. Say it in words.
  • A system’s behaviour comes from the interactions between its parts. Mass or energy may cross the boundary (an open system).
  • Parts can move differently from the whole. Internal structure matters for some questions, and it can change when outside conditions change (water surging in a braking tank).
  • If inner details do not matter, model the system as one object at its center of mass.
  • A uniform symmetric object has its center of mass on its lines of symmetry. The center of mass can be in empty space.

Key relationships

Relationship Units When to use
x_cm = Σmᵢxᵢ / Σmᵢ (same for y, z) m particles, or uniform pieces placed at their own centers
x_cm = ∫x dm / ∫dm m continuous object
λ = dm/dx, so dm = λ dx kg/m rod or other thin object
M = ∫λ dx kg rod with varying density
M = ∫σ dA; M = ∫ρ dV kg plate (σ in kg/m²); solid (ρ in kg/m³)
Hole: include it as a piece of negative mass — composite shapes

Assumptions behind the numbers

  • Thin rods are treated as one-dimensional; plates have negligible thickness.
  • “Uniform” means constant density, so symmetry places the center of mass.
  • Coefficients in a density function carry units: in λ = 0.50 + 1.5x, the 1.5 is in kg/m².

Mistakes to avoid

  1. Dividing by the number of particles instead of the total mass.
  2. Losing the sign of a negative coordinate.
  3. Using λ × length when λ varies. Integrate λ dx.
  4. Stopping at ∫x dm. That has unit kg·m; divide by M.
  5. Assuming half the mass lies on each side of the center of mass.
  6. Insisting the center of mass is on the object. Rings and brackets say otherwise.
  7. Treating every system as a point, even when its internal structure decides the answer.

Quick self-check

  1. A 1.0 kg particle is at (0, 0) and a 3.0 kg particle at (0.40 m, 0.20 m). Where is the center of mass? ((0.30 m, 0.15 m))
  2. A 2.0 m rod has λ = 3.0x (kg/m, x in m from one end). Find M and x_cm. (M = 6.0 kg; x_cm = 4/3 m ≈ 1.3 m)
  3. Where is the center of mass of a uniform thin ring? (At its center, where there is no material.)

Next: practice questions.

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