Choosing Parameterizations - Multivariable Calculus

  1. A curve in 3D space is defined as the intersection of the surfaces x2+y2=4zx^2 + y^2 = 4z and x+y+z=6x + y + z = 6. To parameterize this curve efficiently for computing a line integral, which single-parameter approach is most appropriate?
    Answer: Use the constraint to write z=6−x−yz = 6 - x - y, substitute into x2+y2=4zx^2 + y^2 = 4z to get (x+2)2+(y+2)2=32(x+2)^2 + (y+2)^2 = 32, then parameterize this circle Substituting z=6−x−yz = 6 - x - y into x2+y2=4zx^2 + y^2 = 4z gives x2+y2=4(6−x−y)=24−4x−4yx^2 + y^2 = 4(6-x-y) = 24 - 4x - 4y. Rearranging: x2+4x+y2+4y=24x^2 + 4x + y^2 + 4y = 24. Completing the square: (x+2)2+(y+2)2=24+4+4=32(x+2)^2 + (y+2)^2 = 24 + 4 + 4 = 32. This is a circle with center (−2,−2)(-2, -2) and radius 424\sqrt{2}, parameterized as x=−2+42cos⁡tx = -2 + 4\sqrt{2}\cos t, y=−2+42sin⁡ty = -2 + 4\sqrt{2}\sin t, z=6−x−y=10−42(cos⁡t+sin⁡t)z = 6 - x - y = 10 - 4\sqrt{2}(\cos t + \sin t). Choice A incorrectly assumes the projection is a circle of radius 2. Choice B introduces an unnecessary second parameter. Choice D has an artificial and complicated relationship between parameters that doesn't simplify the problem.
  2. The surface SS is defined by z=ln⁡(x2+y2)z = \ln(x^2 + y^2) for 1≤x2+y2≤e21 \leq x^2 + y^2 \leq e^2. For evaluating ∬Sf(x,y,z) dS\iint_S f(x,y,z)\,dS where ff depends significantly on the distance from the z-axis, which parameterization strategy provides the most computational advantage?
    Answer: Cylindrical: r(r,θ)=(rcos⁡θ,rsin⁡θ,2ln⁡r)\mathbf{r}(r,\theta) = (r\cos\theta, r\sin\theta, 2\ln r) with 1≤r≤e1 \leq r \leq e, 0≤θ≤2π0 \leq \theta \leq 2\pi Since ff depends significantly on the distance from the z-axis (which is x2+y2=r\sqrt{x^2 + y^2} = r), cylindrical coordinates are most appropriate. The surface becomes z=ln⁡(r2)=2ln⁡rz = \ln(r^2) = 2\ln r, so the parameterization is r(r,θ)=(rcos⁡θ,rsin⁡θ,2ln⁡r)\mathbf{r}(r,\theta) = (r\cos\theta, r\sin\theta, 2\ln r) with 1≤r≤e1 \leq r \leq e (since 1≤x2+y2≤e21 \leq x^2 + y^2 \leq e^2 means 1≤r2≤e21 \leq r^2 \leq e^2, so 1≤r≤e1 \leq r \leq e) and 0≤θ≤2π0 \leq \theta \leq 2\pi. This makes the dependence on distance from the z-axis explicit through the parameter rr. Choice A uses Cartesian coordinates which obscures the radial structure. Choice B incorrectly writes z=ln⁡r2z = \ln r^2 without simplifying to 2ln⁡r2\ln r. Choice D introduces an unnecessarily complex substitution that doesn't simplify the problem.
  3. A space curve is defined implicitly as the intersection of x2+z2=9x^2 + z^2 = 9 and y2+z2=9y^2 + z^2 = 9. For parameterizing this curve to compute its arc length, which single-parameter approach avoids issues with undefined derivatives at specific points?
    Answer: Use z=3cos⁡tz = 3\cos t as the parameter, then x=±3sin⁡tx = \pm 3\sin t and y=±3sin⁡ty = \pm 3\sin t, choosing signs to maintain continuity The intersection of x2+z2=9x^2 + z^2 = 9 and y2+z2=9y^2 + z^2 = 9 gives us x2=y2x^2 = y^2, so x=±yx = \pm y. This means the curve consists of two components: one where x=yx = y and one where x=−yx = -y. Both lie on circles of radius 3. Using z=3cos⁡tz = 3\cos t as parameter gives x2=9−z2=9sin⁡2tx^2 = 9 - z^2 = 9\sin^2 t and y2=9−z2=9sin⁡2ty^2 = 9 - z^2 = 9\sin^2 t, so x=±3sin⁡tx = \pm 3\sin t and y=±3sin⁡ty = \pm 3\sin t. To avoid derivative issues, we choose signs consistently for each component. Choice B only captures one component (x=yx = y). Choice C introduces absolute value functions that create derivative discontinuities at t=π2,3π2t = \frac{\pi}{2}, \frac{3\pi}{2}. Choice D also only captures one component and has the same limitation as Choice B.
  4. Consider the surface defined implicitly by x2+y2−z2=1x^2 + y^2 - z^2 = 1 for z≥0z \geq 0. You need to parameterize the portion of this surface where 1≤x2+y2≤41 \leq x^2 + y^2 \leq 4. Which approach provides the most efficient parameterization that avoids singularities?
    Answer: Use cylindrical coordinates: r(r,θ)=(rcos⁡θ,rsin⁡θ,r2−1)\mathbf{r}(r,\theta) = (r\cos\theta, r\sin\theta, \sqrt{r^2-1}) with 1≤r≤21 \leq r \leq 2, 0≤θ≤2π0 \leq \theta \leq 2\pi This is a hyperboloid of one sheet. The constraint 1≤x2+y2≤41 \leq x^2 + y^2 \leq 4 naturally suggests cylindrical coordinates where r=x2+y2r = \sqrt{x^2+y^2}, so 1≤r≤21 \leq r \leq 2. From the surface equation x2+y2−z2=1x^2 + y^2 - z^2 = 1, we get z=r2−1z = \sqrt{r^2-1} (taking positive root since z≥0z \geq 0). This parameterization is well-defined and smooth throughout the domain. Choice B incorrectly uses ρ\rho in place of rr and has wrong bounds. Choice C uses hyperbolic functions which are unnecessarily complex for this region and the bounds are incorrect. Choice D is problematic because it doesn't clearly specify the domain and can lead to computational difficulties when integrating.
  5. You need to parameterize the part of the paraboloid z=x2+y2z = x^2 + y^2 that lies between the cylinders x2+y2=1x^2 + y^2 = 1 and x2+y2=4x^2 + y^2 = 4, but only in the region where x≥∣y∣x \geq |y|. Which parameterization correctly captures this region and is suitable for surface integration?
    Answer: r(r,θ)=(rcos⁡θ,rsin⁡θ,r2)\mathbf{r}(r,\theta) = (r\cos\theta, r\sin\theta, r^2) with 1≤r≤21 \leq r \leq 2 and −π4≤θ≤π4-\frac{\pi}{4} \leq \theta \leq \frac{\pi}{4} or 3π4≤θ≤5π4\frac{3\pi}{4} \leq \theta \leq \frac{5\pi}{4} The condition x≥∣y∣x \geq |y| means x≥yx \geq y when y≥0y \geq 0 and x≥−yx \geq -y when y<0y < 0. In polar coordinates, this corresponds to two angular regions: the first quadrant and parts of the second and fourth quadrants where ∣cos⁡θ∣≥∣sin⁡θ∣|\cos\theta| \geq |\sin\theta|. For θ∈[0,π4]\theta \in [0, \frac{\pi}{4}], we have cos⁡θ≥sin⁡θ≥0\cos\theta \geq \sin\theta \geq 0. For θ∈[−π4,0]\theta \in [-\frac{\pi}{4}, 0], we have cos⁡θ≥−sin⁡θ≥0\cos\theta \geq -\sin\theta \geq 0. By symmetry, we also need θ∈[3π4,5π4]\theta \in [\frac{3\pi}{4}, \frac{5\pi}{4}] to capture the region where x≤0x \leq 0 and x≥∣y∣x \geq |y|. Choice A misses the third quadrant portion. Choice B uses incorrect union notation that suggests simultaneous constraints rather than separate intervals. Choice C uses Cartesian parameterization which is less natural for the annular region and makes integration more complex.
  6. Consider parameterizing the surface z=xyz = xy over the region where x2+y2≤4x^2 + y^2 \leq 4 and x≥0x \geq 0. For computing the flux of the vector field F=zk\mathbf{F} = z\mathbf{k} through this surface, which parameterization choice will result in the normal vector pointing generally upward (positive z-component)?
    Answer: r(x,y)=(x,y,xy)\mathbf{r}(x,y) = (x, y, xy) with x2+y2≤4x^2 + y^2 \leq 4, x≥0x \geq 0, computed as rx×ry\mathbf{r}_x \times \mathbf{r}_y For a surface parameterized as r(u,v)\mathbf{r}(u,v), the normal vector is ru×rv\mathbf{r}_u \times \mathbf{r}_v. For r(x,y)=(x,y,xy)\mathbf{r}(x,y) = (x, y, xy), we have rx=(1,0,y)\mathbf{r}_x = (1, 0, y) and ry=(0,1,x)\mathbf{r}_y = (0, 1, x). Thus rx×ry=(−y,−x,1)\mathbf{r}_x \times \mathbf{r}_y = (-y, -x, 1), which has a positive z-component. Choice A uses the correct region but the cross product rr×rθ\mathbf{r}_r \times \mathbf{r}_{\theta} may not consistently point upward. Choice C computes rv×ru\mathbf{r}_v \times \mathbf{r}_u instead of ru×rv\mathbf{r}_u \times \mathbf{r}_v, which reverses the orientation and gives a downward normal. Choice D parameterizes the wrong half of the disk (x≤0x \leq 0 instead of x≥0x \geq 0).
  7. Consider the curve formed by the intersection of the ellipsoid x24+y29+z216=1\frac{x^2}{4} + \frac{y^2}{9} + \frac{z^2}{16} = 1 and the plane x+2y−z=0x + 2y - z = 0. To parameterize this curve for computing work done by a conservative vector field, which approach most efficiently handles the constraint while maintaining parameter bounds that are easy to determine?
    Answer: Parameterize the plane as p(u,v)=(u,v,u+2v)\mathbf{p}(u,v) = (u, v, u + 2v) and substitute into the ellipsoid equation to find the constraint relating uu and vv, then use this constraint to eliminate one parameter Method C is most systematic. Parameterizing the plane as (u,v,u+2v)(u, v, u + 2v) and substituting into the ellipsoid gives u24+v29+(u+2v)216=1\frac{u^2}{4} + \frac{v^2}{9} + \frac{(u + 2v)^2}{16} = 1. Expanding: u24+v29+u2+4uv+4v216=1\frac{u^2}{4} + \frac{v^2}{9} + \frac{u^2 + 4uv + 4v^2}{16} = 1, which simplifies to 5u216+uv4+25v2144=1\frac{5u^2}{16} + \frac{uv}{4} + \frac{25v^2}{144} = 1. This can be written in the form of an ellipse and parameterized trigonometrically. Choice A leads to a complicated quartic relationship that's difficult to solve explicitly. Choice B introduces two parameters unnecessarily and requires finding a complex relationship between them. Choice D assumes a specific radial form that may not match the actual intersection curve and could lead to rr being multi-valued as a function of θ\theta.

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