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AP Physics C Mechanics uses calculus to describe motion, forces, energy, momentum, rotation, gravitation, and oscillations. This cheat sheet helps students organize the main equations and decide which model fits a problem. It is especially useful for reviewing before quizzes, unit tests, and the AP exam. The formulas connect derivatives, integrals, vectors, and physical meaning.

Key Facts

  • Linear kinematics connects position, velocity, and acceleration by v=dxdtv = \frac{dx}{dt}, a=dvdta = \frac{dv}{dt}, and Δx=t1t2vdt\Delta x = \int_{t_1}^{t_2} v\,dt.
  • Newton's second law is F=ma\sum \vec{F} = m\vec{a} for constant mass, and equilibrium requires F=0\sum \vec{F} = \vec{0}.
  • Work and energy are connected by W=FdrW = \int \vec{F}\cdot d\vec{r} and Wnet=ΔKW_{\text{net}} = \Delta K, where K=12mv2K = \frac{1}{2}mv^2.
  • Linear momentum is p=mv\vec{p} = m\vec{v}, impulse is J=Fdt=Δp\vec{J} = \int \vec{F}\,dt = \Delta \vec{p}, and total momentum is conserved when external impulse is zero.
  • Rotational motion uses ω=dθdt\omega = \frac{d\theta}{dt}, α=dωdt\alpha = \frac{d\omega}{dt}, τ=Iα\tau = I\alpha, and Krot=12Iω2K_{\text{rot}} = \frac{1}{2}I\omega^2.
  • Angular momentum is L=Iω\vec{L} = I\vec{\omega} for rotation about a fixed axis, and L\vec{L} is conserved when the net external torque is zero.
  • Newtonian gravitation uses Fg=Gm1m2r2F_g = \frac{Gm_1m_2}{r^2}, Ug=GMmrU_g = -\frac{GMm}{r}, and circular orbit speed v=GMrv = \sqrt{\frac{GM}{r}}.
  • Simple harmonic motion satisfies a=ω2xa = -\omega^2x, with spring angular frequency ω=km\omega = \sqrt{\frac{k}{m}} and period T=2πmkT = 2\pi\sqrt{\frac{m}{k}}.

Vocabulary

Derivative
A derivative gives an instantaneous rate of change, such as v=dxdtv = \frac{dx}{dt} for velocity.
Integral
An integral accumulates a changing quantity, such as W=FdrW = \int \vec{F}\cdot d\vec{r} for work.
Net Force
Net force is the vector sum of all forces acting on an object, written as F\sum \vec{F}.
Torque
Torque measures the rotational effect of a force and is given by τ=r×F\vec{\tau} = \vec{r}\times \vec{F}.
Moment of Inertia
Moment of inertia II measures how mass is distributed relative to an axis of rotation.
Conservative Force
A conservative force has path-independent work and can be described by potential energy with F=U\vec{F} = -\nabla U.

Common Mistakes to Avoid

  • Using constant-acceleration equations when acceleration is not constant is wrong because equations like v2=v02+2aΔxv^2 = v_0^2 + 2a\Delta x require constant aa.
  • Dropping vector signs in force and momentum problems is wrong because directions determine signs and components in F=ma\sum \vec{F} = m\vec{a} and pi=pf\sum \vec{p}_{i} = \sum \vec{p}_{f}.
  • Confusing work with force is wrong because work depends on displacement and angle through W=FdrW = \int \vec{F}\cdot d\vec{r}.
  • Using τ=rF\tau = rF for every torque problem is wrong because the correct magnitude is τ=rFsinθ\tau = rF\sin\theta or the force times the lever arm.
  • Treating angular momentum as always L=IωL = I\omega is wrong because for a particle the general form is L=r×p\vec{L} = \vec{r}\times \vec{p}.

Practice Questions

  1. 1 A particle moves along the xx-axis with v(t)=3t24tv(t) = 3t^2 - 4t in meters per second. Find its displacement from t=0t = 0 to t=2st = 2\,\text{s}.
  2. 2 A 2.0kg2.0\,\text{kg} block is pulled by a variable force F(x)=5xF(x) = 5x in newtons from x=0x = 0 to x=3.0mx = 3.0\,\text{m}. Find the work done.
  3. 3 A solid disk with I=12MR2I = \frac{1}{2}MR^2 has M=4.0kgM = 4.0\,\text{kg}, R=0.30mR = 0.30\,\text{m}, and ω=12rad/s\omega = 12\,\text{rad/s}. Find its rotational kinetic energy.
  4. 4 A comet speeds up as it falls toward the Sun. Explain why angular momentum can remain constant while kinetic energy changes.