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AP® Physics C: Mechanics · Unit 1 · Topic 1.2

Displacement, Velocity, and Acceleration: Practice Questions (Physics C: Mechanics 1.2)

Seven original Marlbridge calculus-based practice questions on velocity and acceleration as derivatives, integration with initial conditions, derivations and sensor data.

These are original Marlbridge practice questions, not past exam questions. The mark points are a suggested Marlbridge rubric to help you check your work; they are not an official scoring guideline. This set is for the calculus-based Physics C: Mechanics course. In every formula, x is in m, v_x in m/s, a_x in m/s² and t in s, so each numerical coefficient carries whatever unit makes the term correct. Use g = 9.8 m/s² if needed. Round final answers to 2 significant figures unless told otherwise. A calculator is used only for arithmetic.

Question 1 (multiple choice · foundation)

Take +x to the right. A particle’s position is x(t) = 5.0 + 2.0t − 1.0t³. What is its velocity at t = 2.0 s?

  • (A) +0.50 m/s
  • (B) −2.0 m/s
  • (C) −10 m/s
  • (D) −12 m/s
Answer and explanation

Answer: (C). v_x = dx/dt = 2.0 − 3.0t², so v_x(2.0) = 2.0 − 12 = −10 m/s (moving left at 10 m/s).

  • (A) divides position by time: x(2.0) = 1.0 m, and 1.0 m ÷ 2.0 s = 0.50 m/s. Position over clock time is not velocity.
  • (B) is the average velocity from 0 to 2.0 s: (1.0 − 5.0) m ÷ 2.0 s. It is a secant slope, not the instantaneous value.
  • (D) differentiates twice: a_x = −6.0t gives −12 m/s² at 2.0 s. That is the acceleration, with the wrong unit attached.

Question 2 (multiple choice · core)

Take +x to the right. A cart has a_x(t) = 6.0t and an initial velocity v_x0 = −4.0 m/s at t = 0. What is its velocity at t = 2.0 s?

  • (A) +8.0 m/s
  • (B) +12 m/s
  • (C) +16 m/s
  • (D) +20 m/s
Answer and explanation

Answer: (A). v_x = v_x0 + ∫₀ᵗ 6.0t dt = −4.0 + 3.0t². At t = 2.0 s: −4.0 + 12 = +8.0 m/s.

  • (B) leaves out the initial velocity. The integral gives only the change in velocity (+12 m/s).
  • (C) adds the size of v_x0 instead of its signed value: 12 + 4.0. The cart started moving left, so its initial velocity is −4.0 m/s.
  • (D) treats the acceleration as constant at its final value, a_x(2.0) = 12 m/s², for the whole 2.0 s: −4.0 + 12 × 2.0. The acceleration grows from 0, so this overestimates the change.

Question 3 (multiple choice · core)

Take +x to the right. A particle has x(t) = t³ − 6.0t². At t = 1.0 s, which statement is correct?

  • (A) It is speeding up, because v_x and a_x are both negative.
  • (B) It is slowing down, because a_x is negative.
  • (C) It is slowing down, because v_x is negative.
  • (D) It is neither, because x is negative, so the particle is behind the origin.
Answer and explanation

Answer: (A). v_x = 3.0t² − 12t = −9.0 m/s and a_x = 6.0t − 12 = −6.0 m/s² at t = 1.0 s. Both are negative, so velocity and acceleration point the same way and the speed increases.

  • (B) uses the rule “negative acceleration means slowing down”. The sign of a_x alone shows only its direction.
  • (C) confuses moving left with slowing down. A negative velocity means motion in −x.
  • (D) judges motion from position. x = −5.0 m tells you where the particle is, not how its speed is changing.

Question 4 (calculation · core)

Take +x to the right, with the particle at x₀ = 0 at t = 0. Its velocity is v_x(t) = 3.0t² − 12t + 9.0. Find (a) the displacement and (b) the distance travelled from t = 0 to t = 4.0 s.

Worked solution
  1. Integrate: x(t) = 0 + ∫₀ᵗ (3.0t² − 12t + 9.0) dt = t³ − 6.0t² + 9.0t.
  2. (a) Displacement = x(4.0) − x(0) = 64 − 96 + 36 = +4.0 m.
  3. Turning points: v_x = 3.0(t − 1.0)(t − 3.0) = 0 at t = 1.0 s and 3.0 s. Positions: x(1.0) = 4.0 m, x(3.0) = 0, x(4.0) = 4.0 m.
  4. (b) Distance = |4.0 − 0| + |0 − 4.0| + |4.0 − 0| = 4.0 + 4.0 + 4.0 = 12 m.

Suggested mark points (3): 1 for x(t) by integration; 1 for the displacement; 1 for splitting at the turning points and adding the sizes.

Common error: reporting ∫₀⁴ v_x dt = 4.0 m as the distance. That is the displacement; the middle leg moves backwards.

Question 5 (constructed response · core)

Take +x along the motion. A particle has constant acceleration a_x. At t = 0 it is at x₀ with velocity v_x0.

(a) Starting from a_x = dv_x/dt, derive an expression for v_x(t). (b) Use your answer to (a) to derive an expression for x(t). (c) Using the chain rule, derive v_x² = v_x0² + 2a_x(x − x₀). (d) State the condition under which all three results hold, and explain which step of your derivation needs it.

Worked solution and suggested Marlbridge rubric

(a) dv_x = a_x dt. Integrate from (0, v_x0) to (t, v_x): v_x − v_x0 = a_x t, so v_x = v_x0 + a_x t.

(b) dx = v_x dt = (v_x0 + a_x t) dt. Integrate from (0, x₀) to (t, x): x = x₀ + v_x0 t + ½a_x t².

(c) a_x = dv_x/dt = (dv_x/dx)(dx/dt) = v_x (dv_x/dx). So a_x dx = v_x dv_x. Integrate: a_x(x − x₀) = ½(v_x² − v_x0²), giving v_x² = v_x0² + 2a_x(x − x₀).

(d) The acceleration must be constant. In each integral, a_x was taken outside the integral sign (∫a_x dt = a_x t; ∫a_x dx = a_x(x − x₀)). That is only valid if a_x does not change with t or x.

Point What earns it
1 (a) Separates and integrates with the initial condition v_x0
1 (b) Integrates v_x(t) with the initial condition x₀ to reach the quadratic
1 (c) Uses the chain rule to write a_x = v_x dv_x/dx
1 (c) Integrates both sides with correct limits to reach the result
1 (d) States constant acceleration and identifies taking a_x outside the integral as the step that needs it

Alternative methods. For (b), indefinite integrals with a constant found from x(0) = x₀ are equally valid. For (c), eliminating t between (a) and (b) algebraically earns both (c) points if every step is shown, since it still relies on constant a_x.

Question 6 (constructed response · stretch)

Take +x along a level track, origin at the start. A fan cart starts from rest at t = 0. The fan speeds up so that the student predicts a_x = ct, where c is a constant. A motion sensor gives:

t (s) 0.50 1.00 1.50 2.00 2.50
x (m) 0.013 0.100 0.338 0.800 1.563

(a) Show that the prediction gives x = ct³/6. (b) State what to plot against what to obtain a straight line through the origin if the prediction is correct. (c) Use the data to find c, with its unit. (d) Find the cart’s velocity at t = 2.00 s. (e) Describe a second graph that tests the power of t without assuming it is 3.

Worked solution and suggested Marlbridge rubric

(a) v_x = 0 + ∫₀ᵗ ct dt = ct²/2. Then x = 0 + ∫₀ᵗ (ct²/2) dt = ct³/6.

(b) Plot x (m) on the vertical axis against t³ (s³) on the horizontal axis. The prediction gives a straight line through the origin with slope c/6.

(c) Values of t³: 0.125, 1.00, 3.375, 8.00, 15.625 s³. Each x ÷ t³ is about 0.100 m/s³ (for example 0.800 ÷ 8.00 = 0.100), and a best-fit line through the origin also gives slope 0.100 m/s³. So c = 6 × 0.100 = 0.60 m/s³.

(d) v_x = ct²/2 = 0.60 × (2.00)² ÷ 2 = 1.2 m/s.

(e) If x = kt^n, then ln x = ln k + n ln t. Plot ln x against ln t. The slope gives n; these data give a slope of about 3.0, supporting a_x ∝ t. (Plotting log₁₀ x against log₁₀ t works the same way.)

Point What earns it
1 (a) Two integrations, each using the initial condition (starts from rest at the origin)
1 (b) x against t³, with the slope identified as c/6
1 (c) c = 0.60 m/s³ from the slope, with correct unit
1 (d) 1.2 m/s from v_x = ct²/2 (carry forward an incorrect c)
1 (e) Log–log graph with the slope identified as the power of t

Alternative method for (c). Find average velocities between readings, plot them against midpoint times, and fit v_x = ct²/2. This is valid but less precise because the intervals are long; it earns the point if c is within 0.55–0.65 m/s³.

Question 7 (explanation · stretch)

A student says: “For any motion, the average velocity over an interval equals the mean of the starting and ending velocities, (v_x0 + v_x)/2.”

Take +x along the motion. Test the claim for a particle that starts from rest at the origin with a_x = ct (c is a positive constant), over the interval 0 to T. Then state when the claim is true.

Model answer and suggested Marlbridge rubric

Model answer. From Question 6, v_x = ct²/2 and x = ct³/6.

  • True average velocity: v_avg = Δx/Δt = (cT³/6) ÷ T = cT²/6.
  • Mean of end velocities: (0 + cT²/2)/2 = cT²/4.

These differ, so the claim is false in general: the true average is only 2/3 of the student’s value. The particle moves slowly for most of the interval and fast only near the end, so the time-weighted average is lower than the mean of the end values.

The claim is true when acceleration is constant. Then v_x is a linear function of t, the v_x–t graph is a straight line, and the area under it (the displacement) equals Δt × (v_x0 + v_x)/2, the area of a trapezium.

Point What earns it
1 Finds the true average velocity cT²/6 from Δx/Δt
1 Finds the mean of end velocities cT²/4 and concludes the claim fails
1 Explains the difference physically or graphically (more time spent at low speed; curve below the straight chord)
1 States the claim holds for constant acceleration, with the trapezium or linear-v_x reason

A numerical test with a chosen c and T (for example c = 0.60 m/s³ and T = 2.0 s gives 0.40 m/s against 0.60 m/s) earns the first two points.

How did you do?

  • Q1 or Q3 wrong: re-read “From averages to derivatives” and the sign chart in Worked example 1 of the study guide.
  • Q2 or Q4 wrong: revisit “From derivatives back to position” and Worked example 2. Add initial conditions; split at v_x = 0 for distance.
  • Q5 incomplete: go through “Deriving the constant-acceleration equations” step by step.
  • Q6 or Q7 incomplete: your reasoning must say why a graph is straight or why an average differs. Compare with Figure 2 and the failure of constant-a equations in Worked example 2.

Then tick off the topic checklist.

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