AP Calculus BC Practice Quiz: Solving Motion Problems Using Parametric and Vector-Valued Functions
Written by AP Content Team, Verified for 2026 AP Exams, Last updated: May 2026
Test your understanding with short quizzes. This quiz has 9 questions to check your progress.
Question 1 of 9
All Questions (9)
A) <12, π>
B) <12, 0>
C) <6, 0>
D) <11, 1>
Correct Answer: A
To find the velocity vector, we need to find the derivative of each component of the position vector r(t) = <x(t), y(t)>. The velocity vector is v(t) = <x'(t), y'(t)>. Here, x'(t) = 6t and y'(t) = πcos(πt). Evaluating at t = 2, we get x'(2) = 6(2) = 12 and y'(2) = πcos(2π) = π(1) = π. Therefore, the velocity vector at t = 2 is <12, π>. [cite: 3051]
A) <1, 6>
B) <0, 6>
C) <1, 3>
D) <e, 2>
Correct Answer: A
The acceleration vector a(t) is the derivative of the velocity vector v(t). Given v(t) = <ln(t), 2t^3>, we find a(t) = v'(t) = <d/dt(ln(t)), d/dt(2t^3)> = <1/t, 6t^2>. To find the acceleration at t = 1, we substitute t = 1 into the expression for a(t): a(1) = <1/1, 6(1)^2> = <1, 6>. [cite: 3051]
A) 2
B) 4
C) 8
D) 2√3
Correct Answer: B
First, find the velocity vector v(t) = <x'(t), y'(t)>. Here, x'(t) = -4sin(t) and y'(t) = 4cos(t). The speed is the magnitude of the velocity vector, given by the formula speed = ||v(t)|| = sqrt((x'(t))^2 + (y'(t))^2). So, speed = sqrt((-4sin(t))^2 + (4cos(t))^2) = sqrt(16sin^2(t) + 16cos^2(t)) = sqrt(16(sin^2(t) + cos^2(t))) = sqrt(16) = 4. The speed is constant for all t. Therefore, at t = π/3, the speed is 4. [cite: 3051]
A) <8, ln(3)>
B) <12, ln(2)>
C) <8, 3/2>
D) <6, -1/9>
Correct Answer: A
The displacement of the particle is the net change in position, which is found by integrating the velocity vector over the time interval. Displacement = ∫[from 0 to 2] v(t) dt = <∫[from 0 to 2] 3t^2 dt, ∫[from 0 to 2] 1/(t+1) dt>. The x-component is ∫[from 0 to 2] 3t^2 dt = [t^3] from 0 to 2 = 2^3 - 0^3 = 8. The y-component is ∫[from 0 to 2] 1/(t+1) dt = [ln|t+1|] from 0 to 2 = ln(3) - ln(1) = ln(3). Thus, the displacement vector is <8, ln(3)>. [cite: 3052]
A) ∫[from 0 to 2] (t^2 + sin(e^t)) dt
B) ∫[from 0 to 2] sqrt(t^2 + sin^2(e^t)) dt
C) ∫[from 0 to 2] sqrt(4t^2 + e^(2t)cos^2(e^t)) dt
D) ∫[from 0 to 2] sqrt(t^4 + sin^2(e^t)) dt
Correct Answer: D
The total distance traveled by a particle over a time interval [a, b] is the integral of its speed. The speed is the magnitude of the velocity vector, ||v(t)||. Given v(t) = <x'(t), y'(t)> = <t^2, sin(e^t)>, the speed is sqrt((x'(t))^2 + (y'(t))^2) = sqrt((t^2)^2 + (sin(e^t))^2) = sqrt(t^4 + sin^2(e^t)). The total distance traveled from t = 0 to t = 2 is the definite integral of the speed over this interval, which is ∫[from 0 to 2] sqrt(t^4 + sin^2(e^t)) dt. [cite: 3053]
A) (4, 8)
B) (6, 10)
C) (6, 12)
D) (7, 6)
Correct Answer: B
The position at time t=2 can be found by adding the initial position at t=1 to the displacement from t=1 to t=2. The position vector is p(t) = p(1) + ∫[from 1 to 2] v(t) dt. The x-coordinate is x(2) = x(1) + ∫[from 1 to 2] 2t dt = 3 + [t^2] from 1 to 2 = 3 + (2^2 - 1^2) = 3 + 3 = 6. The y-coordinate is y(2) = y(1) + ∫[from 1 to 2] (6t^2 - 2) dt = -2 + [2t^3 - 2t] from 1 to 2 = -2 + [(2(2)^3 - 2(2)) - (2(1)^3 - 2(1))] = -2 + [(16 - 4) - (2 - 2)] = -2 + 12 = 10. The position at t=2 is (6, 10). [cite: 3050, 3052]
A) t = 1
B) t = √3
C) t = 2
D) t = 4
Correct Answer: C
A horizontal tangent line occurs when the vertical component of velocity, dy/dt, is zero, and the horizontal component, dx/dt, is not zero. First, find dy/dt: y'(t) = 2t - 4. Set y'(t) = 0 to find potential times: 2t - 4 = 0, which gives t = 2. Now, we must check that dx/dt is not zero at t = 2. Find dx/dt: x'(t) = 3t^2 - 3. At t = 2, x'(2) = 3(2)^2 - 3 = 12 - 3 = 9. Since x'(2) ≠ 0, the tangent line is horizontal at t = 2. [cite: 3050, 3051]
A) The particle is slowing down.
B) The particle is speeding up.
C) The particle's speed is constant.
D) The particle is at rest.
Correct Answer: B
To determine if the particle is speeding up or slowing down, we can examine the sign of the dot product of the velocity and acceleration vectors, v(t) · a(t). First, find the velocity and acceleration vectors. v(t) = r'(t) = <3t^2, 2t>. a(t) = v'(t) = <6t, 2>. Now, evaluate both at t = 1: v(1) = <3(1)^2, 2(1)> = <3, 2>. a(1) = <6(1), 2> = <6, 2>. Calculate the dot product: v(1) · a(1) = (3)(6) + (2)(2) = 18 + 4 = 22. Since the dot product is positive, the angle between the velocity and acceleration vectors is acute, which means the particle is speeding up. [cite: 3051]
A) 5 + ∫[from 2 to 5] x'(t) dt
B) ∫[from 2 to 5] y'(t) dt
C) 1 + ∫[from 2 to 5] y'(t) dt
D) 1 + ∫[from 2 to 5] sqrt((x'(t))^2 + (y'(t))^2) dt
Correct Answer: C
According to the Fundamental Theorem of Calculus, the final position is the initial position plus the accumulated change (displacement). The displacement in the y-direction from t=2 to t=5 is given by the definite integral of the y-component of velocity, ∫[from 2 to 5] y'(t) dt. To find the y-coordinate at t=5, we add this displacement to the y-coordinate at t=2. Therefore, y(5) = y(2) + ∫[from 2 to 5] y'(t) dt. Since y(2) = 1, the expression is 1 + ∫[from 2 to 5] y'(t) dt. [cite: 3052]