Motion Problems, Parametric, Vector-Valued Functions - AP Calculus BC

  1. A particle moves with x(t)=ln⁡(t+1)x(t)=\ln(t+1) and y(t)=ty(t)=t; what is its speed at t=0t=0?
    Answer: 2\sqrt{2} To find speed, we need the velocity vector components. Differentiating gives vₓ(t) = d/dt[ln(t+1)] = 1/(t+1) and vᵧ(t) = 1. At t = 0, we get vₓ(0) = 1/(0+1) = 1 and vᵧ(0) = 1, so v(0) = ⟨1, 1⟩. The speed is |v(0)| = √(1² + 1²) = √2. Students might report just one component value of 1 (choice A) or the velocity vector itself (choice C). Always remember to find the magnitude of the velocity vector to get speed.
  2. A particle follows r(t)=⟨t−2, (t−2)2⟩r(t)=\langle t-2,\,(t-2)^2\rangle; what is its speed at t=2t=2?
    Answer: 11 This problem involves analyzing the motion of a particle using parametric equations. To find the speed, differentiate: dx/dt = 1 and dy/dt = 2(t-2). At t=2, velocity is <1,0>, and speed is √(1+0)=1. This indicates motion only in the x-direction at that point. A tempting distractor might be √2, perhaps from evaluating at t=1 or t=3 where the y-component is nonzero. Always remember to integrate velocity to find position or differentiate position to find velocity and speed when analyzing parametric motion.
  3. A particle moves as x=t2+1x=t^2+1 and y=4−ty=4-t; what is its velocity at t=3t=3?
    Answer: ⟨6,−1⟩\langle 6,-1\rangle This problem involves analyzing the motion of a particle using parametric equations. To find the velocity, differentiate the given x and y: dx/dt = 2t and dy/dt = -1. At t=3, this yields <6, -1>. The velocity vector shows both components of the motion at that instant. A tempting distractor might be √37, which is the speed instead of the velocity vector. Always remember to integrate velocity to find position or differentiate position to find velocity and speed when analyzing parametric motion.
  4. A particle moves with x(t)=2t−1x(t)=2t-1 and y(t)=t3y(t)=t^3; what is its velocity at t=0t=0?
    Answer: ⟨2,0⟩\langle 2,0\rangle This problem requires finding the velocity vector from parametric equations. The velocity components are found by differentiating: vₓ(t) = dx/dt = 2 and vᵧ(t) = dy/dt = 3t². At t = 0, we get vₓ(0) = 2 and vᵧ(0) = 3(0)² = 0, so v(0) = ⟨2, 0⟩. The particle is moving horizontally to the right at this instant. A student might mistakenly evaluate the position at t = 0 to get ⟨-1, 0⟩ (choice A). Remember that velocity requires differentiation of position, not just evaluation.
  5. A car's position is r(t)=⟨t3, 2t2⟩r(t)=\langle t^3,\,2t^2\rangle; what is its velocity at t=1t=1?
    Answer: ⟨3,4⟩\langle 3,4\rangle This problem involves analyzing the motion of a car using parametric equations. To find the velocity, differentiate: $ dx/dt = 3t23t^2 $ and $ dy/dt = 4t $. At t=1, this is ⟨3,4⟩\langle 3,4 \rangle. The components show the rates in x and y directions. A tempting distractor might be 5, which is the speed 9+16=5\sqrt{9+16} = 5, confusing vector with scalar. Always remember to integrate velocity to find position or differentiate position to find velocity and speed when analyzing parametric motion.
  6. A skater moves with r(t)=⟨3t−1,  t2+2⟩r(t)=\langle 3t-1,\;t^2+2\rangle. What is the speed at t=0t=0?
    Answer: ∣0˘07fr′(0)∣\left|\u007fr'(0)\right| This problem requires finding the speed of a skater at t=0 from parametric equations. Given r(t) = ⟨3t-1, t²+2⟩, we first find the velocity vector: r'(t) = ⟨3, 2t⟩. At t=0, the velocity is r'(0) = ⟨3, 0⟩. Speed is the magnitude of velocity: |r'(0)| = √(3² + 0²) = √9 = 3. Choice B (r'(0) = ⟨3, 0⟩) gives the velocity vector itself, not its magnitude—remember that speed is a scalar quantity. For parametric motion, always compute speed as |r'(t)|, the magnitude of the velocity vector.
  7. For r(t)=⟨t, t2⟩r(t)=\langle t,\,t^2\rangle, what is the displacement vector from t=1t=1 to t=3t=3?
    Answer: ⟨2, 8⟩\langle 2,\,8\rangle This problem involves analyzing the motion of a particle using parametric equations. To find the displacement vector from t = 1 to t = 3, evaluate the position at both times: r(3) = <3, 9> and r(1) = <1, 1>. Subtract the initial position from the final position to get <3 - 1, 9 - 1> = <2, 8>. This vector represents the net change in position over the interval. A tempting distractor is E, √68, which is the magnitude of <2, 8> or the distance traveled, but the question asks for the displacement vector, not its length. A transferable motion-analysis strategy is to compute displacement as the difference in position vectors for any time interval in parametric motion.
  8. A particle has r(t)=⟨1+2t, 5−t⟩r(t)=\langle 1+2t,\,5-t\rangle; what is its speed for any tt?
    Answer: 5\sqrt{5} This problem asks for the speed of a particle with linear parametric equations at any time t. The velocity vector is found by differentiating: v(t)=r′(t)=⟨ddt(1+2t),ddt(5−t)⟩=⟨2,−1⟩v(t) = r'(t) = \langle \frac{d}{dt}(1+2t), \frac{d}{dt}(5-t) \rangle = \langle 2, -1 \rangle. Since the velocity is constant, the speed is also constant: ∣v(t)∣=22+(−1)2=4+1=5|v(t)| = \sqrt{2^2 + (-1)^2} = \sqrt{4 + 1} = \sqrt{5}. Choice A gives the constant velocity vector, not the speed, while choice E attempts a general formula but uses position instead of velocity. For linear parametric equations, velocity is constant, making speed calculation straightforward.
  9. A particle has position r(t)=⟨2cos⁡t, 2sin⁡t⟩r(t)=\langle 2\cos t,\,2\sin t\rangle; which gives its velocity vector at t=π/3t=\pi/3?
    Answer: ⟨−2sin⁡(π/3), 2cos⁡(π/3)⟩\langle -2\sin(\pi/3),\,2\cos(\pi/3)\rangle This problem involves analyzing the motion of a particle using parametric equations. To find the velocity vector, differentiate each component of r(t) = <2 cos t, 2 sin t> with respect to t, resulting in v(t) = <-2 sin t, 2 cos t>. Evaluate at t = π/3, where sin(π/3) = √3/2 and cos(π/3) = 1/2, giving v(π/3) = <-2(√3/2), 2(1/2)> = <-√3, 1>, which matches <-2 sin(π/3), 2 cos(π/3)>. Note that the expression is left in terms of sine and cosine as presented in the choices. A tempting distractor is B, <2 cos(π/3), 2 sin(π/3)>, which is actually the position vector at t = π/3, confusing position with velocity. A transferable motion-analysis strategy is to remember that velocity is the derivative of position, so always apply differentiation to parametric components before evaluation.
  10. A particle's position is r(t)=⟨et, e−t⟩r(t)=\langle e^{t},\,e^{-t}\rangle; what is its speed at t=0t=0?
    Answer: 2\sqrt{2} This problem involves analyzing the motion of a particle using parametric equations. To find the speed at t = 0, differentiate r(t) = ⟨et,e−t⟩\langle e^t, e^{-t} \rangle to obtain v(t) = ⟨et,−e−t⟩\langle e^t, -e^{-t} \rangle. Evaluate at t = 0: v(0) = ⟨1,−1⟩\langle 1, -1 \rangle. The speed is the magnitude 12+(−1)2=2\sqrt{1^2 + (-1)^2} = \sqrt{2}. A tempting distractor is B, 0, which might come from mistakenly thinking the components cancel out without squaring for magnitude. A transferable motion-analysis strategy is to use the magnitude formula after finding velocity to determine speed, especially for exponential parametrizations.
  11. A particle has r(t)=⟨t2, 2t−5⟩r(t)=\langle t^2,\,2t-5\rangle; what is its position at t=2t=2?
    Answer: ⟨4,−1⟩\langle 4,-1\rangle This question simply asks for the position at a specific time. We evaluate the position function at t = 2: r(2) = ⟨2², 2(2) - 5⟩ = ⟨4, 4 - 5⟩ = ⟨4, -1⟩. This is a direct substitution problem. Students might make arithmetic errors, such as getting ⟨4, 1⟩ by incorrectly computing 4 - 5 = 1 (choice B). When finding position at a given time, simply substitute the t-value into both component functions.
  12. A particle's velocity is v(t)=⟨3t2, −4⟩v(t)=\langle 3t^2,\,-4\rangle; what is its speed at t=1t=1?
    Answer: 55 This question asks for speed when velocity is already given. At t = 1, the velocity is v(1) = ⟨3(1)², -4⟩ = ⟨3, -4⟩. Speed is the magnitude of this velocity vector: |v(1)| = √(3² + (-4)²) = √(9 + 16) = √25 = 5. Students might add the components incorrectly to get 7 (choice A) or forget to square before adding. When finding speed from velocity, always use the formula |v| = √(vₓ² + vᵧ²) for the magnitude of the vector.
  13. A robot follows r(t)=⟨cos⁡t, sin⁡t⟩r(t)=\langle \cos t,\,\sin t\rangle; what is its velocity vector at t=π/2t=\pi/2?
    Answer: ⟨−1,0⟩\langle -1,0\rangle This problem involves analyzing the motion of a robot using parametric equations. To find the velocity vector, differentiate the position components: dx/dt=−sin⁡tdx/dt = -\sin t and dy/dt=cos⁡tdy/dt = \cos t. At t=π/2t=\pi/2, this gives ⟨−1,0⟩\langle -1, 0 \rangle. The velocity vector indicates the instantaneous direction and rate of change at that point. A tempting distractor might be ⟨0,1⟩\langle 0,1 \rangle, which is the position at t=π/2t=\pi/2, confusing position with velocity. Always remember to integrate velocity to find position or differentiate position to find velocity and speed when analyzing parametric motion.
  14. For r(t)=⟨3t, sin⁡t⟩r(t)=\langle 3t,\,\sin t\rangle, what is the particle's speed at t=0t=0?
    Answer: 10\sqrt{10} This problem requires finding the speed of a particle with mixed polynomial and trigonometric parametric equations. First, we find the velocity vector by differentiating: v(t)=r′(t)=⟨3,cos⁡t⟩v(t) = r'(t) = \langle 3, \cos t \rangle. At t=0t=0, this becomes v(0)=⟨3,cos⁡(0)⟩=⟨3,1⟩v(0) = \langle 3, \cos(0) \rangle = \langle 3, 1 \rangle. The speed is the magnitude of this velocity vector: ∣v(0)∣=32+12=9+1=10|v(0)| = \sqrt{3^2 + 1^2} = \sqrt{9 + 1} = \sqrt{10}. Choice C gives only the x-component of velocity, ignoring the y-component contribution to speed. For parametric motion, speed requires considering both components of velocity in the magnitude calculation.
  15. A particle moves with r(t)=⟨t3, t2⟩r(t)=\langle t^3,\,t^2\rangle; which is its speed at t=2t=2?
    Answer: 160\sqrt{160} This problem involves analyzing the motion of a particle using parametric equations. To find the speed at t=2t = 2, differentiate r(t)=⟨t3,t2⟩r(t) = \langle t^3, t^2 \rangle to get v(t)=⟨3t2,2t⟩v(t) = \langle 3t^2, 2t \rangle. Evaluate at t=2t = 2: v(2)=⟨3(4),4⟩=⟨12,4⟩v(2) = \langle 3(4), 4 \rangle = \langle 12, 4 \rangle. The speed is the magnitude 122+42=144+16=160\sqrt{12^2 + 4^2} = \sqrt{144 + 16} = \sqrt{160}. A tempting distractor is B, 160, which comes from adding the squares without taking the square root, mistaking it for speed. A transferable motion-analysis strategy is to derive velocity from position derivatives and then find its magnitude to determine speed at any point.
  16. A car's position is r(t)=⟨t3,  4t⟩r(t)=\langle t^3,\;4t\rangle (meters). What is its velocity vector at t=2t=2?
    Answer: ⟨12,  4⟩\langle 12,\;4\rangle This problem requires computing the velocity vector of a car at a specific time using parametric equations. Given r(t) = ⟨t³, 4t⟩, we find velocity by differentiating each component: r'(t) = ⟨3t², 4⟩. At t=2, we substitute to get r'(2) = ⟨3(2)², 4⟩ = ⟨3(4), 4⟩ = ⟨12, 4⟩. The velocity vector tells us both the speed and direction of motion at that instant. Choice C (⟨6, 4⟩) might result from incorrectly computing the derivative as ⟨3t, 4⟩ instead of ⟨3t², 4⟩, a common error when differentiating powers. Always differentiate parametric components carefully: d/dt(tnt^n) = ntn−1nt^{n-1}.
  17. A particle moves with r(t)=⟨1+2t, 4−t⟩r(t)=\langle 1+2t,\,4-t\rangle; which is its velocity vector at t=5t=5?
    Answer: ⟨2,−1⟩\langle 2,-1\rangle For a linear parametric path, the velocity is constant. Differentiating r(t) = ⟨1+2t,4−t⟩\langle 1 + 2t, 4 - t \rangle gives v(t) = ⟨2,−1⟩\langle 2, -1 \rangle for all t. This constant velocity means the particle moves with uniform speed in a fixed direction. Students might substitute t = 5 into the position function to get ⟨11,−1⟩\langle 11, -1 \rangle (choice C) instead of differentiating. For motion problems, always distinguish between position r(t) and velocity v(t) = r'(t).
  18. A swimmer moves with r(t)=⟨1+t2,  3−t⟩r(t)=\langle 1+t^2,\;3-t\rangle. What is the magnitude of velocity at t=2t=2?
    Answer: 17\sqrt{17} This problem requires finding the speed (magnitude of velocity) for a swimmer's parametric motion. Given r(t) = ⟨1+t², 3-t⟩, we differentiate to find velocity: r'(t) = ⟨2t, -1⟩. At t=2, the velocity is r'(2) = ⟨4, -1⟩. The magnitude is |r'(2)| = √(4² + (-1)²) = √(16 + 1) = √17. Choice E (√13) might result from using r'(t) = ⟨2t, -t⟩ instead of ⟨2t, -1⟩, incorrectly differentiating the linear term. When finding speed from parametric equations, carefully differentiate each component before computing the magnitude.
  19. For r(t)=⟨2t−5, t2⟩r(t)=\langle 2t-5,\,t^2\rangle, what is the particle's displacement vector from t=1t=1 to t=3t=3?
    Answer: ⟨4,8⟩\langle 4,8\rangle This problem requires finding the displacement vector for parametric motion over a time interval. Displacement is the change in position vector: Δr=r(3)−r(1)\Delta r = r(3) - r(1). First, we evaluate the position at each time: r(1)=⟨2(1)−5,12⟩=⟨−3,1⟩r(1) = \langle 2(1)-5, 1^2 \rangle = \langle -3, 1 \rangle and r(3)=⟨2(3)−5,32⟩=⟨1,9⟩r(3) = \langle 2(3)-5, 3^2 \rangle = \langle 1, 9 \rangle. The displacement vector is Δr=⟨1,9⟩−⟨−3,1⟩=⟨4,8⟩\Delta r = \langle 1, 9 \rangle - \langle -3, 1 \rangle = \langle 4, 8 \rangle. Choice E incorrectly gives the magnitude of displacement rather than the vector itself. Remember: displacement is a vector quantity showing net change in position, not distance traveled.
  20. A robot's position is r(t)=⟨t,  t2⟩r(t)=\langle t,\;t^2\rangle (meters). Which gives its velocity at t=4t=4?
    Answer: 0˘07fr′(4)\u007fr'(4) This problem asks for the velocity vector of a robot following a parabolic parametric path. Given r(t) = ⟨t, t²⟩, velocity is found by differentiating each component: r'(t) = ⟨1, 2t⟩. This represents the instantaneous rate of change of position. At any time t, including t=4, the velocity vector is r'(t), not its magnitude |r'(t)|. Choice D (|r'(4)|) would give the speed √(1 + 16) = √17, losing the directional information that makes velocity a vector. For parametric motion, velocity r'(t) is a vector quantity that includes both magnitude and direction information.

Start this quiz