Multivariable Calculus Quiz: Triple Integrals Cylindrical
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Triple Integrals CylindricalQuestion 1 of 18

A solid occupies the region bounded by the cylinders x2+y2=1x^2+y^2=1 and x2+y2=4x^2+y^2=4, and the planes z=0z=0 and z=3z=3. The density of the solid at any point (x,y,z)(x,y,z) is inversely proportional to its distance from the zz-axis. If the density is given by ρ(x,y,z)=kx2+y2\rho(x,y,z) = \frac{k}{\sqrt{x^2+y^2}} for some constant kk, what is the total mass of the solid?

6πk6\pi k
6πkln⁡(2)6\pi k \ln(2)
14πk14\pi k
12πk12\pi k
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Multivariable Calculus Quiz

Multivariable Calculus Quiz: Triple Integrals Cylindrical

Practice Triple Integrals Cylindrical in Multivariable Calculus with focused quiz questions that help you check what you know, review explanations, and build confidence with test-style prompts.

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This quiz focuses on Triple Integrals Cylindrical, giving you a quick way to practice the rules, question types, and explanations that matter most for Multivariable Calculus.

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Question 1

A solid occupies the region bounded by the cylinders x2+y2=1x^2+y^2=1 and x2+y2=4x^2+y^2=4, and the planes z=0z=0 and z=3z=3. The density of the solid at any point (x,y,z)(x,y,z) is inversely proportional to its distance from the zz-axis. If the density is given by ρ(x,y,z)=kx2+y2\rho(x,y,z) = \frac{k}{\sqrt{x^2+y^2}} for some constant kk, what is the total mass of the solid?

  1. 6πk6\pi k (correct answer)
  2. 6πkln⁡(2)6\pi k \ln(2)
  3. 14πk14\pi k
  4. 12πk12\pi k
Explanation: In cylindrical coordinates, the region is described by 1≤r≤21 \le r \le 2, 0≤θ≤2π0 \le \theta \le 2\pi, and 0≤z≤30 \le z \le 3. The density function is ρ(r,θ,z)=kr\rho(r, \theta, z) = \frac{k}{r}. The mass is the triple integral of the density. The volume element in cylindrical coordinates is dV=r dz dr dθdV = r \, dz \, dr \, d\theta. M=∭Eρ dV=∫02π∫12∫03(kr)r dz dr dθM = \iiint_E \rho \, dV = \int_0^{2\pi} \int_1^2 \int_0^3 \left(\frac{k}{r}\right) r \, dz \, dr \, d\theta The rr in the density cancels with the rr in the volume element. M=∫02π∫12∫03k dz dr dθ=k∫02π∫12[z]03 dr dθ=k∫02π∫123 dr dθM = \int_0^{2\pi} \int_1^2 \int_0^3 k \, dz \, dr \, d\theta = k \int_0^{2\pi} \int_1^2 [z]_0^3 \, dr \, d\theta = k \int_0^{2\pi} \int_1^2 3 \, dr \, d\theta =3k∫02π[r]12 dθ=3k∫02π(2−1) dθ=3k∫02π1 dθ=3k(2π)=6πk= 3k \int_0^{2\pi} [r]_1^2 \, d\theta = 3k \int_0^{2\pi} (2-1) \, d\theta = 3k \int_0^{2\pi} 1 \, d\theta = 3k(2\pi) = 6\pi k Distractor B arises from forgetting the Jacobian rr in dVdV. Distractor C arises from misinterpreting the density as krkr. Distractor D arises from using incorrect radial limits, such as 00 to 22.

Question 2

Let EE be the solid wedge cut from the cylinder x2+y2≤4x^2+y^2 \le 4 by the planes z=0z=0, z=1z=1, y=0y=0, and y=xy=x, for x≥0x \ge 0. Find the mass of the wedge if the density is given by ρ(x,y,z)=x\rho(x,y,z) = x.

  1. 2\sqrt{2}
  2. 8/38/3
  3. 4(2−2)/34(2-\sqrt{2})/3
  4. 42/34\sqrt{2}/3 (correct answer)
Explanation: The region is described in cylindrical coordinates. The cylinder x2+y2≤4x^2+y^2 \le 4 means 0≤r≤20 \le r \le 2. The planes z=0z=0 and z=1z=1 mean 0≤z≤10 \le z \le 1. The planes y=0y=0 and y=xy=x for x≥0x \ge 0 correspond to angles θ=0\theta=0 and θ=π/4\theta=\pi/4, so 0≤θ≤π/40 \le \theta \le \pi/4. The density is ρ=x=rcos⁡θ\rho=x=r\cos\theta. The mass is the integral of the density: M=∭Ex dV=∫0π/4∫02∫01(rcos⁡θ)⋅r dz dr dθM = \iiint_E x \, dV = \int_0^{\pi/4} \int_0^2 \int_0^1 (r\cos\theta) \cdot r \, dz \, dr \, d\theta =∫0π/4∫02∫01r2cos⁡θ dz dr dθ= \int_0^{\pi/4} \int_0^2 \int_0^1 r^2\cos\theta \, dz \, dr \, d\theta The inner integral (z): ∫01r2cos⁡θ dz=r2cos⁡θ\int_0^1 r^2\cos\theta \, dz = r^2\cos\theta. The middle integral (r): ∫02r2cos⁡θ dr=[r33]02cos⁡θ=83cos⁡θ\int_0^2 r^2\cos\theta \, dr = [\frac{r^3}{3}]_0^2 \cos\theta = \frac{8}{3}\cos\theta. The outer integral (θ\theta): ∫0π/483cos⁡θ dθ=83[sin⁡θ]0π/4=83(22−0)=423\int_0^{\pi/4} \frac{8}{3}\cos\theta \, d\theta = \frac{8}{3}[\sin\theta]_0^{\pi/4} = \frac{8}{3}(\frac{\sqrt{2}}{2} - 0) = \frac{4\sqrt{2}}{3}. Distractor A results from forgetting the Jacobian rr. Distractor B results from using an incorrect angular range, 00 to π/2\pi/2. Distractor C results from using density ρ=y\rho=y instead of ρ=x\rho=x.

Question 3

A solid region EE is bounded by the paraboloid z=x2+y2z = x^2 + y^2 and the plane z=4z = 4. When setting up the triple integral ∭Ef(r,θ,z) dz dr dθ\iiint_E f(r,\theta,z) \, dz \, dr \, d\theta in cylindrical coordinates, what are the correct limits of integration?

  1. ∫02π∫02∫r24f(r,θ,z) dz dr dθ\int_0^{2\pi} \int_0^2 \int_{r^2}^4 f(r,\theta,z) \, dz \, dr \, d\theta (correct answer)
  2. ∫02π∫04∫r24f(r,θ,z) dz dr dθ\int_0^{2\pi} \int_0^4 \int_{r^2}^4 f(r,\theta,z) \, dz \, dr \, d\theta
  3. ∫02π∫02∫0r2f(r,θ,z) dz dr dθ\int_0^{2\pi} \int_0^2 \int_0^{r^2} f(r,\theta,z) \, dz \, dr \, d\theta
  4. ∫0π∫02∫r24f(r,θ,z) dz dr dθ\int_0^{\pi} \int_0^2 \int_{r^2}^4 f(r,\theta,z) \, dz \, dr \, d\theta
Explanation: In cylindrical coordinates, the paraboloid becomes z=r2z = r^2 and the plane is z=4z = 4. The region projects onto a disk in the xyxy-plane where r2≤4r^2 \leq 4, so 0≤r≤20 \leq r \leq 2. For each point (r,θ)(r,\theta), zz ranges from the paraboloid surface z=r2z = r^2 to the plane z=4z = 4. The angle θ\theta goes from 00 to 2π2\pi for the full revolution. Choice B uses incorrect rr limits (should be 2, not 4). Choice C has zz limits reversed. Choice D uses incorrect θ\theta limits (should be 2π2\pi, not π\pi).

Question 4

The integral ∫02π∫02∫02−r2(r2+z2)r dz dr dθ\int_0^{2\pi} \int_0^{\sqrt{2}} \int_0^{2-r^2} (r^2 + z^2) r \, dz \, dr \, d\theta can be split as the sum of two integrals. What is the value of the integral involving only the r2r^2 term?

  1. 8π3\frac{8\pi}{3}
  2. 4π3\frac{4\pi}{3} (correct answer)
  3. 2π3\frac{2\pi}{3}
  4. π3\frac{\pi}{3}
Explanation: When you see a triple integral with a sum in the integrand, you can split it into separate integrals using linearity. This integral is in cylindrical coordinates, where the integrand (r2+z2)r(r^2 + z^2)r becomes r3+rz2r^3 + r z^2 when distributed. For the r2r^2 term (which becomes r3r^3), you need to evaluate: ∫02π∫02∫02−r2r3 dz dr dθ\int_0^{2\pi} \int_0^{\sqrt{2}} \int_0^{2-r^2} r^3 \, dz \, dr \, d\theta Start with the innermost integral: ∫02−r2r3 dz=r3z∣02−r2=r3(2−r2)=2r3−r5\int_0^{2-r^2} r^3 \, dz = r^3z \Big|_0^{2-r^2} = r^3(2-r^2) = 2r^3 - r^5 Next, integrate with respect to rr: ∫02(2r3−r5) dr=[r42−r66]02=48−848=12−16=13\int_0^{\sqrt{2}} (2r^3 - r^5) \, dr = \left[\frac{r^4}{2} - \frac{r^6}{6}\right]_0^{\sqrt{2}} = \frac{4}{8} - \frac{8}{48} = \frac{1}{2} - \frac{1}{6} = \frac{1}{3} Finally, integrate with respect to θ\theta: ∫02π13 dθ=2π3\int_0^{2\pi} \frac{1}{3} \, d\theta = \frac{2\pi}{3} However, choice C gives 2π3\frac{2\pi}{3}, but the correct answer is B: 4π3\frac{4\pi}{3}. Let me recalculate: (2)42−(2)66=42−86=2−43=23\frac{(\sqrt{2})^4}{2} - \frac{(\sqrt{2})^6}{6} = \frac{4}{2} - \frac{8}{6} = 2 - \frac{4}{3} = \frac{2}{3} So the final result is 2π3⋅2=4π3\frac{2\pi}{3} \cdot 2 = \frac{4\pi}{3}. Choice A (8π3\frac{8\pi}{3}) likely comes from computational errors in the power rule. Choice C (2π3\frac{2\pi}{3}) results from the mistake I initially made. Choice D (π3\frac{\pi}{3}) probably stems from errors in the θ\theta integration. Strategy tip: When splitting integrals, work methodically through each variable and double-check your arithmetic with powers—they're easy to miscalculate under pressure.

Question 5

Consider the triple integral ∫0π∫02cos⁡θ∫r24−r2f(r,θ,z) r dz dr dθ\int_0^{\pi} \int_0^{2\cos\theta} \int_{r^2}^{4-r^2} f(r,\theta,z) \, r \, dz \, dr \, d\theta. What constraint must be satisfied for this integral to be well-defined over the entire region of integration?

  1. 2cos⁡θ≥02\cos\theta \geq 0 for all θ∈[0,π]\theta \in [0,\pi], which requires θ≤π2\theta \leq \frac{\pi}{2}
  2. r2≥4−r2r^2 \geq 4-r^2 for all points in the integration region, which requires r≥2r \geq \sqrt{2}
  3. r2≤4−r2r^2 \leq 4-r^2 for all points in the integration region, which requires r≤2r \leq \sqrt{2} (correct answer)
  4. 4−r2≥04-r^2 \geq 0 for all points in the integration region, which requires r≤2r \leq 2
Explanation: When analyzing triple integrals in cylindrical coordinates, you need to ensure all integration bounds are well-defined throughout the entire region. The key is checking that the inner bounds create a valid interval where the lower limit doesn't exceed the upper limit. For this integral to be well-defined, the z-integration bounds must satisfy r2≤4−r2r^2 \leq 4-r^2 at every point in the region. This ensures the lower bound doesn't exceed the upper bound, making the integration interval valid. Solving this inequality: r2≤4−r2r^2 \leq 4-r^2 gives us 2r2≤42r^2 \leq 4, so r2≤2r^2 \leq 2, which means r≤2r \leq \sqrt{2}. This constraint must hold for all valid values of rr in the region. Option A incorrectly focuses on the θ\theta bounds. While 2cos⁡θ2\cos\theta does become negative for θ>π2\theta > \frac{\pi}{2}, this creates issues with the physical interpretation of rr but doesn't directly address what makes the integral well-defined mathematically. Option B has the inequality backwards. If r2≥4−r2r^2 \geq 4-r^2, then the lower z-bound would exceed the upper bound, making the integral undefined. Option D examines 4−r2≥04-r^2 \geq 0, which gives r≤2r \leq 2. While this ensures the upper z-bound is non-negative, it's not the most restrictive condition needed for the integral to be well-defined. Study tip: For triple integrals, always check that integration bounds form valid intervals throughout the region. The most restrictive constraint that ensures all bounds work together is usually the answer.

Question 6

Which of the following describes the solid region of integration for the integral ∫0π/2∫02∫0r2r dz dr dθ\int_{0}^{\pi/2} \int_{0}^{2} \int_{0}^{r^2} r \, dz \, dr \, d\theta

  1. The solid region in the first octant bounded by the cylinder x2+y2=4x^2+y^2=4, the paraboloid z=x2+y2z=x^2+y^2, and the plane z=0z=0. (correct answer)
  2. The solid region bounded by the cone z2=x2+y2z^2=x^2+y^2 and the plane z=4z=4.
  3. The solid region inside the cylinder x2+y2=4x^2+y^2=4 for z≥0z \ge 0, bounded above by the plane z=4z=4 and below by the paraboloid z=x2+y2z=x^2+y^2.
  4. The solid region in the first octant bounded by the sphere x2+y2+z2=4x^2+y^2+z^2=4 and the coordinate planes.
Explanation: Let's analyze the limits of integration. The limits for θ\theta are 00 to π/2\pi/2, which corresponds to the first quadrant in the xyxy-plane. The limits for rr are 00 to 22, which means the projection of the solid onto the xyxy-plane is a quarter-disk of radius 2. This region in the xyxy-plane is bounded by the cylinder x2+y2=4x^2+y^2=4 (since r=2r=2) in the first quadrant. The limits for zz are 00 to r2r^2. The lower bound z=0z=0 is the xyxy-plane. The upper bound z=r2z=r^2 is equivalent to z=x2+y2z=x^2+y^2, which is a paraboloid. Combining these, the integral is over the solid region in the first octant (x≥0,y≥0,z≥0x \ge 0, y \ge 0, z \ge 0) under the paraboloid z=x2+y2z=x^2+y^2 and within the cylinder x2+y2=4x^2+y^2=4. This matches choice A. Choice C describes the region for the integral ∫02π∫02∫r24r dz dr dθ\int_0^{2\pi} \int_0^2 \int_{r^2}^4 r \, dz \, dr \, d\theta. Choice B describes a cone. Choice D describes a portion of a sphere.

Question 7

Evaluate the integral by converting to cylindrical coordinates: ∫−33∫09−x2∫0x2+y2x2+y2 dz dy dx\int_{-3}^{3} \int_{0}^{\sqrt{9-x^2}} \int_{0}^{x^2+y^2} \sqrt{x^2+y^2} \, dz \, dy \, dx

  1. 81π/481\pi/4
  2. 486π/5486\pi/5
  3. 243π/2243\pi/2
  4. 243π/5243\pi/5 (correct answer)
Explanation: The limits of integration in xx and yy describe a semi-disk of radius 3 for y≥0y \ge 0. In cylindrical coordinates, this is 0≤r≤30 \le r \le 3 and 0≤θ≤π0 \le \theta \le \pi. The limits for zz are from 00 to x2+y2=r2x^2+y^2=r^2. The integrand is x2+y2=r\sqrt{x^2+y^2}=r. The volume element is r dz dr dθr \, dz \, dr \, d\theta. The integral becomes: ∫0π∫03∫0r2r⋅r dz dr dθ=∫0π∫03∫0r2r2 dz dr dθ\int_{0}^{\pi} \int_{0}^{3} \int_{0}^{r^2} r \cdot r \, dz \, dr \, d\theta = \int_{0}^{\pi} \int_{0}^{3} \int_{0}^{r^2} r^2 \, dz \, dr \, d\theta Inner integral (z): ∫0r2r2 dz=r2[z]0r2=r4\int_0^{r^2} r^2 \, dz = r^2[z]_0^{r^2} = r^4. Middle integral (r): ∫03r4 dr=[r55]03=2435\int_0^3 r^4 \, dr = [\frac{r^5}{5}]_0^3 = \frac{243}{5}. Outer integral (θ\theta): ∫0π2435 dθ=243π5\int_0^{\pi} \frac{243}{5} \, d\theta = \frac{243\pi}{5}. Distractor A results from forgetting the Jacobian rr. Distractor B results from using the incorrect angular range 00 to 2π2\pi. Distractor C results from incorrectly converting the integrand x2+y2\sqrt{x^2+y^2} to r2r^2.

Question 8

A solid cylinder of radius RR, height HH, and total mass MM has uniform density. Which expression gives its moment of inertia IzI_z about its central axis (the zz-axis)?

  1. MR2MR^2
  2. 12MR2\frac{1}{2}MR^2 (correct answer)
  3. 25MR2\frac{2}{5}MR^2
  4. 14MR2+13MH2\frac{1}{4}MR^2 + \frac{1}{3}MH^2
Explanation: The moment of inertia about the zz-axis is Iz=∭E(x2+y2)ρ dVI_z = \iiint_E (x^2+y^2)\rho \, dV. The density is constant, ρ=MV=MπR2H\rho = \frac{M}{V} = \frac{M}{\pi R^2 H}. In cylindrical coordinates, x2+y2=r2x^2+y^2=r^2, and the region is 0≤r≤R0 \le r \le R, 0≤θ≤2π0 \le \theta \le 2\pi, 0≤z≤H0 \le z \le H. Iz=∫02π∫0R∫0H(r2)ρ⋅r dz dr dθ=ρ∫02π∫0R∫0Hr3 dz dr dθI_z = \int_0^{2\pi} \int_0^R \int_0^H (r^2)\rho \cdot r \, dz \, dr \, d\theta = \rho \int_0^{2\pi} \int_0^R \int_0^H r^3 \, dz \, dr \, d\theta Inner integral (z): r3Hr^3 H. Middle integral (r): ∫0Rr3H dr=H[r44]0R=HR44\int_0^R r^3 H \, dr = H[\frac{r^4}{4}]_0^R = \frac{HR^4}{4}. Outer integral (θ\theta): ∫02πHR44 dθ=HR44(2π)=πρHR42\int_0^{2\pi} \frac{HR^4}{4} \, d\theta = \frac{HR^4}{4}(2\pi) = \frac{\pi \rho H R^4}{2}. Substituting ρ=MπR2H\rho = \frac{M}{\pi R^2 H}: Iz=πHR42(MπR2H)=12MR2I_z = \frac{\pi H R^4}{2} \left( \frac{M}{\pi R^2 H} \right) = \frac{1}{2}MR^2 Distractor A is the moment of inertia of a thin hoop. Distractor C is for a solid sphere. Distractor D is the moment of inertia of the cylinder about a diameter through its center.

Question 9

The volume of the solid bounded by the paraboloid z=x2+y2z=x^2+y^2 and the plane z=hz=h is 18π18\pi. What is the value of the positive constant hh?

  1. 3
  2. 6 (correct answer)
  3. 323\sqrt{2}
  4. 3233\sqrt[3]{2}
Explanation: The solid is bounded by z=r2z=r^2 and z=hz=h. The intersection occurs when r2=hr^2=h, so r=hr=\sqrt{h}. The volume is given by the integral: V=∫02π∫0h∫r2hr dz dr dθV = \int_0^{2\pi} \int_0^{\sqrt{h}} \int_{r^2}^{h} r \, dz \, dr \, d\theta Inner integral (z): r(h−r2)=hr−r3r(h-r^2) = hr-r^3. Middle integral (r): ∫0h(hr−r3) dr=[hr22−r44]0h=h(h)2−h24=h22−h24=h24\int_0^{\sqrt{h}} (hr-r^3) \, dr = [\frac{hr^2}{2} - \frac{r^4}{4}]_0^{\sqrt{h}} = \frac{h(h)}{2} - \frac{h^2}{4} = \frac{h^2}{2} - \frac{h^2}{4} = \frac{h^2}{4}. Outer integral (θ\theta): ∫02πh24 dθ=h24(2π)=πh22\int_0^{2\pi} \frac{h^2}{4} \, d\theta = \frac{h^2}{4}(2\pi) = \frac{\pi h^2}{2}. We are given that the volume is 18π18\pi. So, πh22=18π\frac{\pi h^2}{2} = 18\pi. This simplifies to h2=36h^2 = 36, and since hh is positive, h=6h=6. Distractor A, h=3h=3, results from an error in the rr integral, getting h2/2h^2/2 instead of h2/4h^2/4. Distractor C, h=32h=3\sqrt{2}, results from forgetting the Jacobian rr.

Question 10

Find the mass of the solid that lies within the cylinder x2+y2=4x^2+y^2=4, below the plane z=y+3z=y+3, and above the plane z=0z=0, given that the density is ρ(x,y,z)=z\rho(x,y,z)=z.

  1. 12π12\pi
  2. 18π18\pi
  3. 20π20\pi (correct answer)
  4. 22π22\pi
Explanation: We need to compute M=∭Ez dVM = \iiint_E z \, dV. In cylindrical coordinates, the region is 0≤r≤20 \le r \le 2, 0≤θ≤2π0 \le \theta \le 2\pi, and 0≤z≤rsin⁡θ+30 \le z \le r\sin\theta+3. The mass integral is: M=∫02π∫02∫0rsin⁡θ+3z⋅r dz dr dθM = \int_0^{2\pi} \int_0^2 \int_0^{r\sin\theta+3} z \cdot r \, dz \, dr \, d\theta Inner integral (z): r[z22]0rsin⁡θ+3=r2(rsin⁡θ+3)2=r2(r2sin⁡2θ+6rsin⁡θ+9)r[\frac{z^2}{2}]_0^{r\sin\theta+3} = \frac{r}{2}(r\sin\theta+3)^2 = \frac{r}{2}(r^2\sin^2\theta + 6r\sin\theta + 9). Middle integral (r): 12∫02(r3sin⁡2θ+6r2sin⁡θ+9r) dr=12[r44sin⁡2θ+2r3sin⁡θ+9r22]02=12(4sin⁡2θ+16sin⁡θ+18)=2sin⁡2θ+8sin⁡θ+9\frac{1}{2}\int_0^2 (r^3\sin^2\theta + 6r^2\sin\theta + 9r) \, dr = \frac{1}{2}[\frac{r^4}{4}\sin^2\theta + 2r^3\sin\theta + \frac{9r^2}{2}]_0^2 = \frac{1}{2}(4\sin^2\theta + 16\sin\theta + 18) = 2\sin^2\theta + 8\sin\theta + 9. Outer integral (θ\theta), using sin⁡2θ=1−cos⁡(2θ)2\sin^2\theta = \frac{1-\cos(2\theta)}{2}: ∫02π(2sin⁡2θ+8sin⁡θ+9) dθ=∫02π(1−cos⁡(2θ)+8sin⁡θ+9) dθ\int_0^{2\pi} (2\sin^2\theta + 8\sin\theta + 9) \, d\theta = \int_0^{2\pi} (1-\cos(2\theta) + 8\sin\theta + 9) \, d\theta =∫02π(10−cos⁡(2θ)+8sin⁡θ) dθ=[10θ−12sin⁡(2θ)−8cos⁡θ]02π=20π= \int_0^{2\pi} (10 - \cos(2\theta) + 8\sin\theta) \, d\theta = [10\theta - \frac{1}{2}\sin(2\theta) - 8\cos\theta]_0^{2\pi} = 20\pi Distractor A is the volume of the solid. Distractor B is the result if the plane were z=3z=3. Distractor D results from an error in integrating sin⁡2θ\sin^2\theta.

Question 11

Find the volume of the solid bounded below by the cone z=x2+y2z=\sqrt{x^2+y^2} and above by the paraboloid z=6−x2−y2z=6-x^2-y^2.

  1. 16π3\frac{16\pi}{3}
  2. 32π3\frac{32\pi}{3} (correct answer)
  3. 16π16\pi
  4. 44π3\frac{44\pi}{3}
Explanation: To find the volume, we set up a triple integral in cylindrical coordinates. The cone is z=rz=r and the paraboloid is z=6−r2z=6-r^2. The intersection of these surfaces occurs when r=6−r2r = 6-r^2, which gives r2+r−6=0r^2+r-6=0, or (r+3)(r−2)=0(r+3)(r-2)=0. Since r≥0r \ge 0, we have r=2r=2. This is the radius of the projection of the solid onto the xyxy-plane. The volume integral is: V=∫02π∫02∫r6−r2r dz dr dθV = \int_{0}^{2\pi} \int_{0}^{2} \int_{r}^{6-r^2} r \, dz \, dr \, d\theta The inner integral with respect to zz is ∫r6−r2r dz=r[z]r6−r2=r(6−r2−r)=6r−r3−r2\int_{r}^{6-r^2} r \, dz = r[z]_{r}^{6-r^2} = r(6-r^2-r) = 6r-r^3-r^2. The middle integral is ∫02(6r−r3−r2) dr=[3r2−r44−r33]02=12−4−83=163\int_{0}^{2} (6r-r^3-r^2) \, dr = [3r^2 - \frac{r^4}{4} - \frac{r^3}{3}]_{0}^{2} = 12 - 4 - \frac{8}{3} = \frac{16}{3}. The outer integral is ∫02π163 dθ=163(2π)=32π3\int_{0}^{2\pi} \frac{16}{3} \, d\theta = \frac{16}{3}(2\pi) = \frac{32\pi}{3}.

Question 12

What is the average value of the function f(x,y,z)=zf(x,y,z) = z over the cylindrical solid bounded by x2+y2≤9x^2+y^2 \le 9, z=0z=0, and z=5z=5?

  1. 5/35/3
  2. 22
  3. 5/25/2 (correct answer)
  4. 55
Explanation: The average value of a function ff over a region EE is given by 1V∭Ef dV\frac{1}{V} \iiint_E f \, dV, where VV is the volume of EE. The region is a cylinder with radius r=3r=3 and height h=5h=5. Its volume is V=πr2h=π(32)(5)=45πV = \pi r^2 h = \pi(3^2)(5) = 45\pi. We need to compute the integral of f(x,y,z)=zf(x,y,z)=z over this region in cylindrical coordinates. The integral is: ∭Ez dV=∫02π∫03∫05z⋅r dz dr dθ\iiint_E z \, dV = \int_0^{2\pi} \int_0^3 \int_0^5 z \cdot r \, dz \, dr \, d\theta Integrating with respect to zz: ∫05zr dz=r[z22]05=25r2\int_0^5 zr \, dz = r[\frac{z^2}{2}]_0^5 = \frac{25r}{2}. Integrating with respect to rr: ∫0325r2 dr=252[r22]03=252(92)=2254\int_0^3 \frac{25r}{2} \, dr = \frac{25}{2}[\frac{r^2}{2}]_0^3 = \frac{25}{2}(\frac{9}{2}) = \frac{225}{4}. Integrating with respect to θ\theta: ∫02π2254 dθ=2254(2π)=225π2\int_0^{2\pi} \frac{225}{4} \, d\theta = \frac{225}{4}(2\pi) = \frac{225\pi}{2}. The average value is 225π/245π=22590=52\frac{225\pi/2}{45\pi} = \frac{225}{90} = \frac{5}{2}. Distractor A, 5/35/3, results from forgetting the Jacobian rr in the integral. Distractor D, 55, is the maximum value of the function, not the average. Distractor B, 22, is a plausible arithmetic error.

Question 13

Which of the following integrals represents the volume of the solid region in the first octant bounded by the cylinder x2+y2=9x^2+y^2=9, the plane z=0z=0, and the plane z=yz=y?

  1. ∫02π∫03∫0rsin⁡θr dz dr dθ\int_0^{2\pi} \int_0^3 \int_0^{r\sin\theta} r \, dz \, dr \, d\theta
  2. ∫0π/2∫03∫0rsin⁡θ dz dr dθ\int_0^{\pi/2} \int_0^3 \int_0^{r\sin\theta} \, dz \, dr \, d\theta
  3. ∫0π/2∫03∫0yr dz dr dθ\int_0^{\pi/2} \int_0^3 \int_0^{y} r \, dz \, dr \, d\theta
  4. ∫0π/2∫03∫0rsin⁡θr dz dr dθ\int_0^{\pi/2} \int_0^3 \int_0^{r\sin\theta} r \, dz \, dr \, d\theta (correct answer)
Explanation: The solid is in the first octant, so x≥0,y≥0,z≥0x \ge 0, y \ge 0, z \ge 0. This corresponds to an angle range of 0≤θ≤π/20 \le \theta \le \pi/2. The cylinder x2+y2=9x^2+y^2=9 means the radius goes from 00 to 33, so 0≤r≤30 \le r \le 3. The solid is bounded below by z=0z=0 and above by z=yz=y. In cylindrical coordinates, y=rsin⁡θy=r\sin\theta, so the zz limits are 0≤z≤rsin⁡θ0 \le z \le r\sin\theta. The volume element is dV=r dz dr dθdV = r \, dz \, dr \, d\theta. Combining these gives the integral: V=∫0π/2∫03∫0rsin⁡θr dz dr dθV = \int_0^{\pi/2} \int_0^3 \int_0^{r\sin\theta} r \, dz \, dr \, d\theta Choice A uses the wrong angular range (00 to 2π2\pi). Choice B is missing the Jacobian factor rr in the volume element. Choice C incorrectly mixes Cartesian variable yy in the limits of an integral with respect to zz where yy is not a variable of integration.

Question 14

A solid of uniform density is bounded by the paraboloid z=x2+y2z=x^2+y^2 and the plane z=4z=4. Find the zz-coordinate of its center of mass, zˉ\bar{z}.

  1. 22
  2. 12/512/5
  3. 16/316/3
  4. 8/38/3 (correct answer)
Explanation: The center of mass for a uniform density solid is its centroid. By symmetry, xˉ=yˉ=0\bar{x}=\bar{y}=0. We need to find zˉ=MxyV\bar{z} = \frac{M_{xy}}{V}. In cylindrical coordinates, the region is bounded by z=r2z=r^2 and z=4z=4. The intersection is at r=2r=2. The volume is V=∫02π∫02∫r24r dz dr dθ=2π∫02r(4−r2) dr=2π[2r2−r44]02=2π(8−4)=8πV = \int_0^{2\pi}\int_0^2\int_{r^2}^4 r \, dz \, dr \, d\theta = 2\pi \int_0^2 r(4-r^2) \, dr = 2\pi [2r^2 - \frac{r^4}{4}]_0^2 = 2\pi(8-4) = 8\pi. The moment about the xyxy-plane is Mxy=∭Ez dV=∫02π∫02∫r24z⋅r dz dr dθ=2π∫02r[z22]r24 dr=π∫02r(16−r4) dr=π[8r2−r66]02=π(32−646)=π(32−323)=64π3M_{xy} = \iiint_E z \, dV = \int_0^{2\pi}\int_0^2\int_{r^2}^4 z \cdot r \, dz \, dr \, d\theta = 2\pi \int_0^2 r[\frac{z^2}{2}]_{r^2}^4 \, dr = \pi \int_0^2 r(16-r^4) \, dr = \pi [8r^2 - \frac{r^6}{6}]_0^2 = \pi(32 - \frac{64}{6}) = \pi(32 - \frac{32}{3}) = \frac{64\pi}{3}. Then zˉ=64π/38π=83\bar{z} = \frac{64\pi/3}{8\pi} = \frac{8}{3}. Distractor A is the midpoint of the zz-interval, a naive guess. Distractor B, 12/512/5, is the result of forgetting the Jacobian rr in both the volume and moment calculations. Distractor C, 16/316/3, is obtained if one makes an error integrating zz, using ∫z dz=z2\int z \, dz = z^2 instead of z2/2z^2/2.

Question 15

The triple integral ∫02π∫03∫09−r2r dz dr dθ\int_0^{2\pi} \int_0^3 \int_0^{9-r^2} r \, dz \, dr \, d\theta represents the volume of which solid region?

  1. The region inside the cylinder x2+y2=9x^2 + y^2 = 9 and below the paraboloid z=9−x2−y2z = 9 - x^2 - y^2, above the xyxy-plane (correct answer)
  2. The region inside the cylinder x2+y2=3x^2 + y^2 = 3 and below the paraboloid z=9−x2−y2z = 9 - x^2 - y^2, above the xyxy-plane
  3. The region inside the cylinder x2+y2=9x^2 + y^2 = 9 and above the paraboloid z=x2+y2−9z = x^2 + y^2 - 9, below the plane z=0z = 0
  4. The region inside the sphere x2+y2+z2=9x^2 + y^2 + z^2 = 9 and below the paraboloid z=9−x2−y2z = 9 - x^2 - y^2
Explanation: The limits show 0≤r≤30 \leq r \leq 3 and 0≤z≤9−r20 \leq z \leq 9-r^2. Since r2=x2+y2r^2 = x^2 + y^2, the region is inside the cylinder x2+y2≤9x^2 + y^2 \leq 9 (radius 3, so x2+y2=9x^2 + y^2 = 9 is the boundary). The zz limits go from 0 to 9−r2=9−x2−y29-r^2 = 9-x^2-y^2, which is a downward-opening paraboloid. Choice B incorrectly states the cylinder equation. Choice C has the wrong paraboloid orientation. Choice D incorrectly describes a spherical boundary.

Question 16

To evaluate ∭Ez dV\iiint_E z \, dV where EE is the region bounded by z=x2+y2z = \sqrt{x^2 + y^2} and z=2z = 2, which integral in cylindrical coordinates is correct?

  1. ∫02π∫02∫r2z dz dr dθ\int_0^{2\pi} \int_0^2 \int_r^2 z \, dz \, dr \, d\theta
  2. ∫02π∫04∫r2z⋅r dz dr dθ\int_0^{2\pi} \int_0^4 \int_r^2 z \cdot r \, dz \, dr \, d\theta
  3. ∫02π∫02∫0rz⋅r dz dr dθ\int_0^{2\pi} \int_0^2 \int_0^r z \cdot r \, dz \, dr \, d\theta
  4. ∫02π∫02∫r2z⋅r dz dr dθ\int_0^{2\pi} \int_0^2 \int_r^2 z \cdot r \, dz \, dr \, d\theta (correct answer)
Explanation: When converting triple integrals to cylindrical coordinates, you need to carefully identify the region of integration and remember the key transformation: dV=r dr dθ dzdV = r \, dr \, d\theta \, dz. The region E is bounded by the cone z=x2+y2z = \sqrt{x^2 + y^2} (which becomes z=rz = r in cylindrical coordinates) and the plane z=2z = 2. This creates a cone-shaped region where the cone opens upward from the origin, and we're looking at the portion between the cone surface and the horizontal plane at z=2z = 2. For the integration limits: θ\theta ranges from 00 to 2π2\pi (full rotation), rr ranges from 00 to 22 (since at z=2z = 2, the cone has radius 22), and for each fixed (r,θ)(r,\theta), zz ranges from the cone surface z=rz = r up to the plane z=2z = 2. The integrand zz stays as zz, and we must include the Jacobian factor rr. Answer D correctly captures all these elements: ∫02π∫02∫r2z⋅r dz dr dθ\int_0^{2\pi} \int_0^2 \int_r^2 z \cdot r \, dz \, dr \, d\theta. Answer A omits the crucial Jacobian factor rr. Answer B has the wrong upper limit for rr (should be 22, not 44). Answer C has the zz-limits backwards—zz should go from rr (the cone) up to 22 (the plane), not from 00 to rr. Study tip: Always remember the cylindrical coordinate Jacobian rr, and sketch the region to verify your integration bounds match the geometry.

Question 17

A region EE is defined by the inequalities x2+y2≤2yx^2 + y^2 \leq 2y and 0≤z≤x2+y20 \leq z \leq x^2 + y^2. When setting up ∭EdV\iiint_E dV in cylindrical coordinates, what are the correct limits?

  1. ∫02π∫02sin⁡θ∫0r2r dz dr dθ\int_0^{2\pi} \int_0^{2\sin\theta} \int_0^{r^2} r \, dz \, dr \, d\theta
  2. ∫0π∫02sin⁡θ∫0r2r dz dr dθ\int_0^{\pi} \int_0^{2\sin\theta} \int_0^{r^2} r \, dz \, dr \, d\theta (correct answer)
  3. ∫0π∫02cos⁡θ∫0r2r dz dr dθ\int_0^{\pi} \int_0^{2\cos\theta} \int_0^{r^2} r \, dz \, dr \, d\theta
  4. ∫0π/2∫02sin⁡θ∫0r2r dz dr dθ\int_0^{\pi/2} \int_0^{2\sin\theta} \int_0^{r^2} r \, dz \, dr \, d\theta
Explanation: When converting triple integrals to cylindrical coordinates, you need to carefully analyze the region's boundaries and convert each constraint from Cartesian to cylindrical form using x=rcos⁡θx = r\cos\theta, y=rsin⁡θy = r\sin\theta, and z=zz = z. Start with the constraint x2+y2≤2yx^2 + y^2 \leq 2y. In cylindrical coordinates, this becomes r2≤2rsin⁡θr^2 \leq 2r\sin\theta. Dividing by rr (assuming r>0r > 0), you get r≤2sin⁡θr \leq 2\sin\theta. This describes a circle in the xyxy-plane. For 2sin⁡θ2\sin\theta to be non-negative (since r≥0r \geq 0), you need sin⁡θ≥0\sin\theta \geq 0, which means 0≤θ≤π0 \leq \theta \leq \pi. The zz-constraint 0≤z≤x2+y20 \leq z \leq x^2 + y^2 becomes 0≤z≤r20 \leq z \leq r^2 in cylindrical coordinates. Therefore, the correct setup is ∫0π∫02sin⁡θ∫0r2r dz dr dθ\int_0^{\pi} \int_0^{2\sin\theta} \int_0^{r^2} r \, dz \, dr \, d\theta, which is option B. Option A uses θ\theta from 00 to 2π2\pi, but for π<θ<2π\pi < \theta < 2\pi, sin⁡θ<0\sin\theta < 0, making the upper limit 2sin⁡θ2\sin\theta negative, which is invalid for the radial coordinate. Option C incorrectly uses 2cos⁡θ2\cos\theta instead of 2sin⁡θ2\sin\theta—this would correspond to the constraint x2+y2≤2xx^2 + y^2 \leq 2x, not 2y2y. Option D restricts θ\theta to [0,π/2][0, \pi/2], which only covers the first quadrant and misses the second quadrant portion of the region. Remember: always check that your angular limits ensure non-negative radial bounds, and carefully distinguish between constraints involving xx versus yy when converting to cylindrical coordinates.

Question 18

When converting the triple integral ∫02∫04−x2∫x2+y24f(x,y,z) dz dy dx\int_0^2 \int_0^{\sqrt{4-x^2}} \int_{x^2+y^2}^4 f(x,y,z) \, dz \, dy \, dx to cylindrical coordinates, which of the following represents the correct conversion?

  1. ∫0π∫02∫r24f(rcos⁡θ,rsin⁡θ,z)⋅r dz dr dθ\int_0^{\pi} \int_0^2 \int_{r^2}^4 f(r\cos\theta, r\sin\theta, z) \cdot r \, dz \, dr \, d\theta
  2. ∫0π/2∫02∫r24f(rcos⁡θ,rsin⁡θ,z) dz dr dθ\int_0^{\pi/2} \int_0^2 \int_{r^2}^4 f(r\cos\theta, r\sin\theta, z) \, dz \, dr \, d\theta
  3. ∫0π/2∫02∫r24f(rcos⁡θ,rsin⁡θ,z)⋅r dz dr dθ\int_0^{\pi/2} \int_0^2 \int_{r^2}^4 f(r\cos\theta, r\sin\theta, z) \cdot r \, dz \, dr \, d\theta (correct answer)
  4. ∫02π∫02∫r24f(rcos⁡θ,rsin⁡θ,z)⋅r dz dr dθ\int_0^{2\pi} \int_0^2 \int_{r^2}^4 f(r\cos\theta, r\sin\theta, z) \cdot r \, dz \, dr \, d\theta
Explanation: When converting triple integrals from Cartesian to cylindrical coordinates, you need to carefully analyze both the region of integration and remember the coordinate transformation rules. Let's examine the original integral's region. The limits show: 0≤x≤20 \leq x \leq 2, 0≤y≤4−x20 \leq y \leq \sqrt{4-x^2}, and x2+y2≤z≤4x^2+y^2 \leq z \leq 4. The condition y≤4−x2y \leq \sqrt{4-x^2} with x,y≥0x,y \geq 0 describes the first quadrant of a circle with radius 2, since x2+y2≤4x^2 + y^2 \leq 4. In cylindrical coordinates, we use x=rcos⁡θx = r\cos\theta, y=rsin⁡θy = r\sin\theta, and z=zz = z. The Jacobian determinant is rr, so we must include this factor in our integral. The function becomes f(rcos⁡θ,rsin⁡θ,z)f(r\cos\theta, r\sin\theta, z). For the limits: Since we're only in the first quadrant, θ\theta ranges from 00 to π/2\pi/2. The radius rr goes from 00 to 22 (the circle's radius). The zz-limits x2+y2x^2+y^2 to 44 become r2r^2 to 44 since r2=x2+y2r^2 = x^2 + y^2. Answer C is correct because it has the proper θ\theta range (00 to π/2\pi/2), includes the essential Jacobian factor rr, and has correct limits for all variables. Answer A uses θ\theta from 00 to π\pi (half a circle, not just first quadrant). Answer B omits the crucial Jacobian factor rr. Answer D uses θ\theta from 00 to 2π2\pi (full circle instead of first quadrant). Study tip: Always identify the geometric region first, then systematically convert each component: limits, function, and don't forget the Jacobian!