Motion from Parametric Graphs - Calculus 3

  1. A particle moves along the curve r⃗(t)=⟨etcos⁡(3t),etsin⁡(3t)⟩\vec{r}(t) = \langle e^t \cos(3t), e^t \sin(3t) \rangle for t≥0t \geq 0. Which property of the motion remains constant throughout the particle's trajectory?
    Answer: The angle between the velocity vector and the position vector remains constant at arctan⁡(3)\arctan(3) We have r⃗(t)=et⟨cos⁡(3t),sin⁡(3t)⟩\vec{r}(t) = e^t\langle \cos(3t), \sin(3t) \rangle and v⃗(t)=et⟨cos⁡(3t)−3sin⁡(3t),sin⁡(3t)+3cos⁡(3t)⟩\vec{v}(t) = e^t\langle \cos(3t) - 3\sin(3t), \sin(3t) + 3\cos(3t) \rangle. To find the angle between r⃗\vec{r} and v⃗\vec{v}, compute cos⁡(θ)=r⃗⋅v⃗∣r⃗∣∣v⃗∣\cos(\theta) = \frac{\vec{r} \cdot \vec{v}}{|\vec{r}||\vec{v}|}. We get r⃗⋅v⃗=e2t[cos⁡(3t)(cos⁡(3t)−3sin⁡(3t))+sin⁡(3t)(sin⁡(3t)+3cos⁡(3t))]=e2t[1]=e2t\vec{r} \cdot \vec{v} = e^{2t}[\cos(3t)(\cos(3t) - 3\sin(3t)) + \sin(3t)(\sin(3t) + 3\cos(3t))] = e^{2t}[1] = e^{2t}. Also, ∣r⃗∣=et|\vec{r}| = e^t and ∣v⃗∣=et(cos⁡(3t)−3sin⁡(3t))2+(sin⁡(3t)+3cos⁡(3t))2=et1+9=et10|\vec{v}| = e^t\sqrt{(\cos(3t) - 3\sin(3t))^2 + (\sin(3t) + 3\cos(3t))^2} = e^t\sqrt{1 + 9} = e^t\sqrt{10}. Thus cos⁡(θ)=e2tet⋅et10=110\cos(\theta) = \frac{e^{2t}}{e^t \cdot e^t\sqrt{10}} = \frac{1}{\sqrt{10}}, so θ=arccos⁡(110)=arctan⁡(3)\theta = \arccos\left(\frac{1}{\sqrt{10}}\right) = \arctan(3). Choice A gives the wrong constant value. Choice C and D describe properties that vary with time.
  2. A particle follows the parametric path x(t)=t3−3tx(t) = t^3 - 3t, y(t)=t2−1y(t) = t^2 - 1 for −2≤t≤2-2 \leq t \leq 2. At how many distinct points along this path does the particle instantaneously move in a direction perpendicular to the line connecting that point to the origin?
    Answer: Exactly two points, occurring at parameter values where the velocity vector is orthogonal to the position vector Motion perpendicular to the line from origin requires r⃗(t)⊥v⃗(t)\vec{r}(t) \perp \vec{v}(t), so r⃗(t)⋅v⃗(t)=0\vec{r}(t) \cdot \vec{v}(t) = 0. We have r⃗(t)=⟨t3−3t,t2−1⟩\vec{r}(t) = \langle t^3 - 3t, t^2 - 1 \rangle and v⃗(t)=⟨3t2−3,2t⟩\vec{v}(t) = \langle 3t^2 - 3, 2t \rangle. Setting r⃗⋅v⃗=(t3−3t)(3t2−3)+(t2−1)(2t)=0\vec{r} \cdot \vec{v} = (t^3 - 3t)(3t^2 - 3) + (t^2 - 1)(2t) = 0. Expanding: 3(t3−3t)(t2−1)+2t(t2−1)=(t2−1)[3(t3−3t)+2t]=(t2−1)(3t3−9t+2t)=(t2−1)(3t3−7t)=t(t2−1)(3t2−7)=03(t^3 - 3t)(t^2 - 1) + 2t(t^2 - 1) = (t^2 - 1)[3(t^3 - 3t) + 2t] = (t^2 - 1)(3t^3 - 9t + 2t) = (t^2 - 1)(3t^3 - 7t) = t(t^2 - 1)(3t^2 - 7) = 0. This gives t=0t = 0, t=±1t = \pm 1, and t=±7/3≈±1.53t = \pm\sqrt{7/3} \approx \pm 1.53. All solutions are in the domain [−2,2][-2, 2]. However, we need to check which correspond to distinct geometric points. Since the parametric equations don't create self-intersections for these parameter values, we have exactly two distinct geometric points where this perpendicularity condition is satisfied.
  3. A particle's position is given by r⃗(t)=⟨t2−4t,sin⁡(πt)⟩\vec{r}(t) = \langle t^2 - 4t, \sin(\pi t) \rangle for t≥0t \geq 0. During which time interval is the particle moving southeast (both velocity components negative) while decelerating?
    Answer: 1<t<21 < t < 2 Southeast motion requires both x′(t)<0x'(t) < 0 and y′(t)<0y'(t) < 0. We have v⃗(t)=⟨2t−4,πcos⁡(πt)⟩\vec{v}(t) = \langle 2t - 4, \pi\cos(\pi t) \rangle. For x′(t)=2t−4<0x'(t) = 2t - 4 < 0, we need t<2t < 2. For y′(t)=πcos⁡(πt)<0y'(t) = \pi\cos(\pi t) < 0, we need cos⁡(πt)<0\cos(\pi t) < 0, which occurs when 12<t<32\frac{1}{2} < t < \frac{3}{2}, 52<t<72\frac{5}{2} < t < \frac{7}{2}, etc. The intersection of t<2t < 2 and 12<t<32\frac{1}{2} < t < \frac{3}{2} gives 12<t<32\frac{1}{2} < t < \frac{3}{2}. Deceleration requires v⃗⋅a⃗<0\vec{v} \cdot \vec{a} < 0. With a⃗(t)=⟨2,−π2sin⁡(πt)⟩\vec{a}(t) = \langle 2, -\pi^2\sin(\pi t) \rangle, we get v⃗⋅a⃗=(2t−4)(2)+πcos⁡(πt)(−π2sin⁡(πt))=4t−8−π3cos⁡(πt)sin⁡(πt)\vec{v} \cdot \vec{a} = (2t-4)(2) + \pi\cos(\pi t)(-\pi^2\sin(\pi t)) = 4t - 8 - \pi^3\cos(\pi t)\sin(\pi t). For 1<t<321 < t < \frac{3}{2}, we have 4t−8<−24t - 8 < -2 and cos⁡(πt)<0\cos(\pi t) < 0, sin⁡(πt)>0\sin(\pi t) > 0, so the second term is positive, making the entire expression negative, confirming deceleration.

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