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AP Physics C: Mechanics — Practice Questions flashcards

6 of 50 questions free to study here · 7 topics · the whole deck is built into Willys

Multiple-choice practice questions, one best answer each, on calculus-based kinematics, drag, gravitation, work and potential energy, momentum, rotation and oscillations.

Practice deck · part of AP Physics C: Mechanics · written against: College Board AP Physics C: Mechanics Course and Exam Description (2024 revision). Updated 2026-10-10.

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  1. A particle moves along the x-axis with velocity v(t)=3t2−12v(t) = 3t^2 - 12 (m/s, t in seconds). At t=0t = 0 it is at x=5x = 5 m. Where is it at t=3t = 3 s?

    A) x=−4x = -4 m
    B) x=12x = 12 m
    C) x=−9x = -9 m
    D) x=20x = 20 m
    A) x=−4x = -4 m

    Position is the starting point plus the integral of velocity: x=5+∫03(3t2−12)dt=5+(27−36)=−4x = 5 + \int_0^3 \left(3t^2 - 12\right) dt = 5 + \left(27 - 36\right) = -4 m. Leaving out the initial position gives −9-9 m.
    Kinematics
  2. A thin rod lies along the x-axis from x=0x = 0 to x=Lx = L⁠. Its linear mass density is λ=Cx2\lambda = Cx^2⁠, where C is a positive constant. Where is its center of mass?

    A) x=2L3x = \frac{2L}{3}
    B) x=L2x = \frac{L}{2}
    C) x=3L4x = \frac{3L}{4}
    D) x=L3x = \frac{L}{3}
    C) x=3L4x = \frac{3L}{4}

    xcm=∫xλdx∫λdx=CL4/4CL3/3=3L4x_{cm} = \frac{\int x\lambda dx}{\int \lambda dx} = \frac{CL^4/4}{CL^3/3} = \frac{3L}{4}⁠. The value 2L3\frac{2L}{3} belongs to a density proportional to xx⁠, not x2x^2⁠.
    Force and Translational Dynamics › Center of Mass
  3. A force along the x-axis is F(x)=12−3x2F(x) = 12 - 3x^2 (newtons, x in meters). How much work does it do on an object that moves from x=0x = 0 to x=2x = 2 m?

    A) 16 J
    B) 12 J
    C) 0 J
    D) 24 J
    A) 16 J

    W=∫02(12−3x2)dx=24−8=16W = \int_0^2 \left(12 - 3x^2\right) dx = 24 - 8 = 16 J. 24 J assumes the force stays at its initial 12 N over the whole 2 m.
    Work Energy and Power › Work and Power
  4. A turbine starts from rest with angular acceleration α(t)=4t\alpha(t) = 4t (rad/s², t in seconds). Through what angle does it turn in the first 3.0 s?

    A) 18 rad
    B) 27 rad
    C) 36 rad
    D) 54 rad
    A) 18 rad

    Integrate twice: ω=2t2\omega = 2t^2 and θ=2t33=18\theta = \frac{2t^3}{3} = 18 rad at t=3t = 3 s. Treating α(3)=12\alpha(3) = 12 rad/s² as constant gives 12(12)(3)2=54\frac{1}{2}\left(12\right)\left(3\right)^2 = 54 rad.
    Torque and Rotational Dynamics › Rotational Kinematics
  5. A thin-walled hollow sphere (I=23MR2I = \frac{2}{3}MR^2⁠) rolls without slipping from rest down a ramp, dropping a vertical height h. What is its speed at the bottom?

    A) 10gh7\sqrt{\frac{10gh}{7}}
    B) 2gh\sqrt{2gh}
    C) gh\sqrt{gh}
    D) 6gh5\sqrt{\frac{6gh}{5}}
    D) 6gh5\sqrt{\frac{6gh}{5}}

    Mgh=12Mv2(1+23)Mgh = \frac{1}{2}Mv^2\left(1 + \frac{2}{3}\right)⁠, so v=6gh5v = \sqrt{\frac{6gh}{5}}⁠. 10gh7\sqrt{\frac{10gh}{7}} is the solid-sphere result, and 2gh\sqrt{2gh} ignores rotational kinetic energy.
    Energy and Momentum of Rotating Systems › Rotational Energy and Rolling
  6. An oscillator's position is x(t)=0.10cos⁡(4t+π3)x(t) = 0.10\cos\left(4t + \frac{\pi}{3}\right) (meters, seconds). What is its velocity at t=0t = 0⁠?

    A) −0.20 m/s
    B) −0.40 m/s
    C) −0.35 m/s
    D) +0.35 m/s
    C) −0.35 m/s

    v=dxdt=−0.40sin⁡(4t+π3)v = \frac{dx}{dt} = -0.40\sin\left(4t + \frac{\pi}{3}\right)⁠, which is −0.40⋅32≈−0.35-0.40\cdot\frac{\sqrt{3}}{2} \approx -0.35 m/s at t=0t = 0⁠. −0.40 m/s would mean moving at the maximum speed, 0.40 m/s, which is reached only at equilibrium.
    Oscillations

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  • Topic outline follows the College Board AP Physics C: Mechanics Course and Exam Description (2024 revised framework, Units 1–7); the AP name is used nominatively and no course or exam text is reproduced.
  • OpenStax University Physics Volume 1, consulted as a reference; no text copied.

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