Velocity and Acceleration β€” Question 3

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Question 3

A particle satisfies 𝒂(t)=⟨6t,4e2t,βˆ’2⟩,𝒗(0)=⟨1,βˆ’1,3⟩,𝒓(0)=⟨2,0,βˆ’4⟩.\mathbf a(t)=\left\langle 6t,\ 4e^{2t},\ -2\right\rangle,\qquad \mathbf v(0)=\left\langle 1,-1,3\right\rangle,\qquad \mathbf r(0)=\left\langle 2,0,-4\right\rangle. Tasks

  1. Recover 𝒗(t)\mathbf v(t).

  2. Recover 𝒓(t)\mathbf r(t).

  3. Verify both initial conditions and the acceleration.

Original worksheet page 1: question and worked solution for 1-11-003
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Question 3 – Solution

Strategy. Integrate componentwise twice, determining a new constant vector at each stage.

Step 1: Velocity 𝒗(t)=⟨3t2+C1,2e2t+C2,βˆ’2t+C3⟩.\mathbf v(t)=\left\langle 3t^2+C_1,2e^{2t}+C_2,-2t+C_3\right\rangle. At t=0t=0, comparison with ⟨1,βˆ’1,3⟩\left\langle 1,-1,3\right\rangle gives C1=1,2+C2=βˆ’1,C3=3.C_1=1,\qquad 2+C_2=-1,\qquad C_3=3. Therefore 𝒗(t)=⟨3t2+1,2e2tβˆ’3,3βˆ’2t⟩.\boxed{\mathbf v(t)=\left\langle 3t^2+1,2e^{2t}-3,3-2t\right\rangle}.

Step 2: Position Integrating velocity, 𝒓(t)=⟨t3+t+D1,e2tβˆ’3t+D2,3tβˆ’t2+D3⟩.\mathbf r(t)=\left\langle t^3+t+D_1,e^{2t}-3t+D_2,3t-t^2+D_3\right\rangle. Using 𝒓(0)=⟨2,0,βˆ’4⟩\mathbf r(0)=\left\langle 2,0,-4\right\rangle gives D1=2D_1=2, 1+D2=01+D_2=0, and D3=βˆ’4D_3=-4. Hence 𝒓(t)=⟨t3+t+2,e2tβˆ’3tβˆ’1,3tβˆ’t2βˆ’4⟩.\boxed{\mathbf r(t)=\left\langle t^3+t+2,e^{2t}-3t-1,3t-t^2-4\right\rangle}.

Step 3: Verification Differentiating 𝒓\mathbf r gives the displayed 𝒗\mathbf v; differentiating again gives ⟨6t,4e2t,βˆ’2⟩\left\langle 6t,4e^{2t},-2\right\rangle. Direct substitution at t=0t=0 returns both required initial vectors.

Original worksheet page 2: question and worked solution for 1-11-003

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