Vector-Valued Functions - Calculus 3

  1. Consider the vector-valued function F⃗(t)=⟨tcos⁡(t),tsin⁡(t),t2⟩\vec{F}(t) = \langle t\cos(t), t\sin(t), t^2 \rangle. The curve traced by this function from t=0t = 0 to t=2πt = 2\pi most closely resembles which geometric shape?
    Answer: A spiral cone with increasing radius and increasing pitch The parametric equations show that in the xy-plane, we have x=tcos⁡(t)x = t\cos(t) and y=tsin⁡(t)y = t\sin(t), which gives x2+y2=t\sqrt{x^2 + y^2} = t. This means the distance from the z-axis increases linearly with the parameter tt, creating an expanding spiral. Meanwhile, z=t2z = t^2 increases quadratically, so the vertical spacing between successive turns increases as we move up. This describes a spiral cone with increasing radius and increasing pitch. Choice A is wrong because the radius increases (not constant). Choice B is wrong because the pitch increases (z=t2z = t^2, not linear). Choice D is wrong because the radius increases (not decreases) and the height increment increases (not constant).
  2. A parametric curve is defined by r⃗(t)=⟨t3−6t,t2⟩\vec{r}(t) = \langle t^3 - 6t, t^2 \rangle for t∈Rt \in \mathbb{R}. At how many distinct points does this curve intersect itself?
    Answer: 1 Self-intersections occur when r⃗(t1)=r⃗(t2)\vec{r}(t_1) = \vec{r}(t_2) for t1≠t2t_1 \neq t_2. This means t13−6t1=t23−6t2t_1^3 - 6t_1 = t_2^3 - 6t_2 and t12=t22t_1^2 = t_2^2. From the second equation, either t1=t2t_1 = t_2 (which we exclude) or t1=−t2t_1 = -t_2. Substituting t2=−t1t_2 = -t_1 into the first equation: t13−6t1=(−t1)3−6(−t1)=−t13+6t1t_1^3 - 6t_1 = (-t_1)^3 - 6(-t_1) = -t_1^3 + 6t_1. This gives 2t13−12t1=02t_1^3 - 12t_1 = 0, so 2t1(t12−6)=02t_1(t_1^2 - 6) = 0. Thus t1=0,±6t_1 = 0, \pm\sqrt{6}. For t1=0t_1 = 0, we get t2=0t_2 = 0 (same point). For t1=6t_1 = \sqrt{6}, we get t2=−6t_2 = -\sqrt{6}, giving the intersection point (63−66,6)=(−56,6)(\sqrt{6}^3 - 6\sqrt{6}, 6) = (-5\sqrt{6}, 6). Similarly for t1=−6t_1 = -\sqrt{6}, we get the same point. Therefore, there is exactly 1 self-intersection.
  3. The vector-valued function r⃗(t)=⟨ln⁡(t2+1),arctan⁡(t),tt2+1⟩\vec{r}(t) = \langle \ln(t^2 + 1), \arctan(t), \frac{t}{\sqrt{t^2 + 1}} \rangle is defined for all real tt. Which of the following statements about this curve is true?
    Answer: The curve is unbounded in the xx-direction but bounded in both yy and zz directions Let's analyze each component: For the xx-component: ln⁡(t2+1)→∞\ln(t^2 + 1) \to \infty as t→±∞t \to \pm\infty, so it's unbounded above and bounded below by ln⁡(1)=0\ln(1) = 0. For the yy-component: arctan⁡(t)\arctan(t) has range (−π2,π2)(-\frac{\pi}{2}, \frac{\pi}{2}), so it's bounded. For the zz-component: tt2+1\frac{t}{\sqrt{t^2 + 1}} approaches ±1\pm 1 as t→±∞t \to \pm\infty (since tt2+1=t/∣t∣1+1/t2→±1\frac{t}{\sqrt{t^2 + 1}} = \frac{t/|t|}{\sqrt{1 + 1/t^2}} \to \pm 1), so it has range (−1,1)(-1, 1) and is bounded. Therefore, the curve is unbounded only in the xx-direction. Choice A is wrong because it's not bounded in all directions. Choice C is wrong because the zz-component is bounded. Choice D is wrong because only the xx-component is unbounded.
  4. Consider the parametric curve r⃗(t)=⟨acos⁡3(t),asin⁡3(t)⟩\vec{r}(t) = \langle a\cos^3(t), a\sin^3(t) \rangle where a>0a > 0. This curve is known as an astroid. What is the total arc length of one complete astroid (0≤t≤2π0 \leq t \leq 2\pi)?
    Answer: 6a6a When you encounter arc length problems for parametric curves, you need to use the formula L=∫ab(dxdt)2+(dydt)2 dtL = \int_a^b \sqrt{\left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2} \, dt. For this astroid, let's find the derivatives first. Given r⃗(t)=⟨acos⁡3(t),asin⁡3(t)⟩\vec{r}(t) = \langle a\cos^3(t), a\sin^3(t) \rangle, we have: - dxdt=−3acos⁡2(t)sin⁡(t)\frac{dx}{dt} = -3a\cos^2(t)\sin(t) - dydt=3asin⁡2(t)cos⁡(t)\frac{dy}{dt} = 3a\sin^2(t)\cos(t) The integrand becomes: 9a2cos⁡4(t)sin⁡2(t)+9a2sin⁡4(t)cos⁡2(t)=3a∣cos⁡(t)sin⁡(t)∣cos⁡2(t)+sin⁡2(t)=3a∣cos⁡(t)sin⁡(t)∣\sqrt{9a^2\cos^4(t)\sin^2(t) + 9a^2\sin^4(t)\cos^2(t)} = 3a|\cos(t)\sin(t)|\sqrt{\cos^2(t) + \sin^2(t)} = 3a|\cos(t)\sin(t)| Since the astroid has four-fold symmetry, you can calculate the arc length for one quadrant (0≤t≤π20 \leq t \leq \frac{\pi}{2}) and multiply by 4. In this interval, both cos⁡(t)\cos(t) and sin⁡(t)\sin(t) are non-negative, so: L=4∫0π/23acos⁡(t)sin⁡(t) dt=12a∫0π/2cos⁡(t)sin⁡(t) dtL = 4 \int_0^{\pi/2} 3a\cos(t)\sin(t) \, dt = 12a \int_0^{\pi/2} \cos(t)\sin(t) \, dt Using substitution u=sin⁡(t)u = \sin(t), du=cos⁡(t)dtdu = \cos(t)dt: L=12a∫01u du=12a⋅12=6aL = 12a \int_0^1 u \, du = 12a \cdot \frac{1}{2} = 6a This confirms answer A is correct. Answer B (4πa4\pi a) and C (3πa3\pi a) incorrectly assume the arc length involves π\pi, likely from confusing this with circular arc formulas. Answer D (8a8a) might result from computational errors in the integration or symmetry analysis. Study tip: For parametric curves with clear symmetry like astroids, always exploit that symmetry to simplify your integration limits and avoid sign complications with absolute values.
  5. Consider the space curve r⃗(t)=⟨2cos⁡(3t),2sin⁡(3t),4sin⁡(t)⟩\vec{r}(t) = \langle 2\cos(3t), 2\sin(3t), 4\sin(t) \rangle. What is the period of this parametric curve (i.e., the smallest positive value TT such that r⃗(t+T)=r⃗(t)\vec{r}(t+T) = \vec{r}(t) for all tt)?
    Answer: 2π2\pi When finding the period of a parametric curve, you need to determine when all components return to their starting values simultaneously. This requires finding the least common multiple of the individual periods of each trigonometric function. Let's analyze each component of r⃗(t)=⟨2cos⁡(3t),2sin⁡(3t),4sin⁡(t)⟩\vec{r}(t) = \langle 2\cos(3t), 2\sin(3t), 4\sin(t) \rangle: - The xx-component 2cos⁡(3t)2\cos(3t) has period 2π3\frac{2\pi}{3} (since cos⁡(3t)\cos(3t) completes one cycle when 3t=2π3t = 2\pi) - The yy-component 2sin⁡(3t)2\sin(3t) also has period 2π3\frac{2\pi}{3} - The zz-component 4sin⁡(t)4\sin(t) has period 2π2\pi For the entire curve to repeat, all components must return to their starting values. This happens at the least common multiple of 2π3\frac{2\pi}{3} and 2π2\pi. Since 2π=3⋅2π32\pi = 3 \cdot \frac{2\pi}{3}, the LCM is 2π2\pi. We can verify: at t+2πt + 2\pi, we have cos⁡(3(t+2π))=cos⁡(3t+6π)=cos⁡(3t)\cos(3(t + 2\pi)) = \cos(3t + 6\pi) = \cos(3t) and sin⁡(t+2π)=sin⁡(t)\sin(t + 2\pi) = \sin(t). Answer choice A (2π3\frac{2\pi}{3}) is just the period of the xx and yy components, but ignores the zz-component. Choice B (π\pi) doesn't work since cos⁡(3t+3π)=−cos⁡(3t)\cos(3t + 3\pi) = -\cos(3t). Choice C (6π6\pi) is a multiple of the true period but not the smallest one. Study tip: For parametric curves with multiple trigonometric functions, always find the LCM of all individual periods—don't just focus on one component.

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