Shell Method - Calculus 2

  1. A solid is formed by revolving the region bounded by the curve y=x−x4y=x-x^4 and the x-axis about the y-axis. Setting up the volume integral using the washer method would be difficult because it requires solving for xx in terms of yy. Which integral correctly sets up the volume using the more convenient shell method?
    Answer: ∫012πx(x−x4) dx\int_0^1 2\pi x(x-x^4) \,dx To use the shell method for revolution about the y-axis (a vertical axis), we integrate with respect to xx. The intersection points of y=x−x4y=x-x^4 and y=0y=0 are x(1−x3)=0x(1-x^3)=0, so x=0x=0 and x=1x=1. These are the limits of integration. The radius of a cylindrical shell is the distance from the y-axis, so r(x)=xr(x)=x. The height of the shell is the function value, h(x)=x−x4h(x) = x-x^4. The volume is V=∫012πr(x)h(x) dx=∫012πx(x−x4) dxV = \int_0^1 2\pi r(x)h(x) \,dx = \int_0^1 2\pi x(x-x^4) \,dx.
  2. A region is bounded by y=2xy = 2x, y=6y = 6, and x=0x = 0. When revolved around the yy-axis, both the shell method and disk/washer method can be used. If the shell method gives volume VsV_s and requires evaluating ∫03f(x)dx\int_0^3 f(x) dx, what is f(x)f(x)?
    Answer: f(x)=2πx(6−2x)f(x) = 2\pi x(6 - 2x) When using the shell method to find volumes of revolution around the y-axis, you're essentially summing up cylindrical shells with radius xx, height determined by the function, and thickness dxdx. The general formula is V=2π∫x⋅(height) dxV = 2\pi \int x \cdot (\text{height}) \, dx. First, let's understand this region. The boundaries are y=2xy = 2x, y=6y = 6, and x=0x = 0. These intersect at (0,0)(0,0), (3,6)(3,6), and (0,6)(0,6), forming a triangle. When you slice this region with vertical strips (for the shell method), each strip at position xx extends from y=2xy = 2x up to y=6y = 6, giving a height of 6−2x6 - 2x. For the shell method around the y-axis, the volume is Vs=2π∫03x(6−2x) dxV_s = 2\pi \int_0^3 x(6 - 2x) \, dx. This means f(x)=2πx(6−2x)f(x) = 2\pi x(6 - 2x), which is answer C. Let's examine why the other options are wrong. Option A, f(x)=x(6−2x)f(x) = x(6 - 2x), gives you just the area element without the 2π2\pi factor required for the shell method volume formula. Option B, f(x)=πx2(6−2x)f(x) = \pi x^2(6 - 2x), incorrectly uses π\pi instead of 2π2\pi and has an extra factor of xx, suggesting confusion with the disk method. Option D, f(x)=2πx2(6−2x)f(x) = 2\pi x^2(6 - 2x), has the correct 2π2\pi but includes an extra xx factor. Remember: shell method integrands always have the form 2π×radius×height2\pi \times \text{radius} \times \text{height}, where radius is the distance from the axis of rotation.
  3. Let R be the region bounded by y=ex2y=e^{x^2}, y=0y=0, x=0x=0, and x=1x=1. When revolving R about the y-axis, the shell method is preferable. If the volume is approximated by nn cylindrical shells of equal thickness, what is the volume of the ii-th shell (where xix_i is the right endpoint of the ii-th subinterval)?
    Answer: Vi=2πnxiexi2V_i = \frac{2\pi}{n} x_i e^{x_i^2} The interval [0,1][0,1] is divided into nn subintervals of thickness Δx=1/n\Delta x = 1/n. The right endpoint of the ii-th interval is xi=i/nx_i = i/n. For the shell method, the volume of the ii-th shell is approximated by 2πrihiΔx2\pi r_i h_i \Delta x. Here, the radius is ri=xir_i = x_i and the height is hi=exi2h_i = e^{x_i^2}. The thickness is Δx=1/n\Delta x = 1/n. So, the volume of the ii-th shell is Vi=2πxiexi2Δx=2π(i/n)e(i/n)2(1/n)=2πin2e(i/n)2V_i = 2\pi x_i e^{x_i^2} \Delta x = 2\pi (i/n) e^{(i/n)^2} (1/n) = \frac{2\pi i}{n^2} e^{(i/n)^2}. Option B uses xix_i instead of i/ni/n, which is a more general representation: Vi=2πxiexi2(1/n)=2πnxiexi2V_i = 2\pi x_i e^{x_i^2} (1/n) = \frac{2\pi}{n} x_i e^{x_i^2}. Let's re-examine C. It's 2πin2e(i/n)2\frac{2\pi i}{n^2} e^{(i/n)^2}. This matches my derivation. Let's check B again. 2πnxiexi2=2πn(i/n)e(i/n)2=2πin2e(i/n)2\frac{2\pi}{n} x_i e^{x_i^2} = \frac{2\pi}{n} (i/n) e^{(i/n)^2} = \frac{2\pi i}{n^2} e^{(i/n)^2}. So B and C are equivalent if we substitute xi=i/nx_i=i/n. B is a slightly better form. I will choose B. The key is 2πrhΔx2\pi r h \Delta x.
  4. The integral ∫022π(4−y)(y/2)dy\int_0^2 2\pi(4-y)(y/2) dy represents the volume of a solid of revolution. If the same volume is to be calculated using the washer method, what would be the integral?
    Answer: ∫01π(42−(4−2x)2)dx\int_0^1 \pi(4^2 - (4-2x)^2) dx From the shell integral (wrt yy), we identify the components. Axis of revolution: horizontal, from radius r(y)=4−yr(y)=4-y, so the axis is y=4y=4. Height of shell: h(y)=y/2h(y)=y/2, so x=y/2x=y/2 is the curve. The region is a triangle bounded by x=y/2x=y/2 (or y=2xy=2x), x=0x=0 (from h(y)h(y) at y=0y=0) and y=2y=2 (upper limit). When y=2y=2, x=1x=1. The region is bounded by y=2xy=2x, y=2y=2 and x=0x=0. For the washer method (wrt xx for horizontal axis), the integration is from x=0x=0 to x=1x=1. The outer radius is the distance from y=4y=4 to the bottom curve y=2xy=2x, so R(x)=4−2xR(x)=4-2x. The inner radius is the distance from y=4y=4 to the top curve y=2y=2, so r(x)=4−2=2r(x)=4-2=2. The integral is V=∫01π((4−2x)2−22)dxV = \int_0^1 \pi((4-2x)^2 - 2^2)dx. This does not match C. Let's re-read the shell integral. h(y)=y/2h(y)=y/2. Limits y=0y=0 to y=2y=2. Region is bounded by x=y/2x=y/2, x=0x=0, y=0y=0, y=2y=2. Axis y=4y=4. Washer method: xx from 0 to 1. Outer radius from y=4y=4 to y=0y=0, R=4R=4. Inner radius from y=4y=4 to y=2xy=2x, r=4−2xr=4-2x. So V=∫01π(42−(4−2x)2)dxV=\int_0^1 \pi(4^2-(4-2x)^2)dx. This matches C.
  5. The region bounded by y=x2−1y = x^2 - 1 and y=3y=3 is revolved about the y-axis. Which integral gives the volume of the resulting solid?
    Answer: ∫−13π(y+1)2 dy\int_{-1}^3 \pi (\sqrt{y+1})^2 \,dy This problem can be solved by either the shell or washer method. The washer method is more direct. Revolving around the y-axis means integrating with respect to yy. The region spans from y=−1y=-1 to y=3y=3. The curve is x2=y+1x^2=y+1, so x=±y+1x=\pm\sqrt{y+1}. The radius of a washer at height yy is R(y)=y+1R(y)=\sqrt{y+1}. The volume is V=∫−13πR(y)2 dy=∫−13π(y+1)2 dyV = \int_{-1}^3 \pi R(y)^2 \,dy = \int_{-1}^3 \pi (\sqrt{y+1})^2 \,dy. Using the shell method requires care because the radius must be positive; the integral is ∫−222π∣x∣(3−(x2−1)) dx=∫−222π∣x∣(4−x2) dx\int_{-2}^2 2\pi |x|(3-(x^2-1)) \,dx = \int_{-2}^2 2\pi |x|(4-x^2) \,dx. Note that ∫−222πx(4−x2) dx=0\int_{-2}^2 2\pi x(4-x^2) \,dx = 0 because the integrand is an odd function over a symmetric interval.
  6. The region bounded by x=y2x = y^2, x=0x=0, and y=2y=2 is revolved around the line y=3y=3. Which integral gives the volume of the resulting solid using the shell method?
    Answer: V=∫022π(3−y)(y2) dyV = \int_0^2 2\pi (3-y)(y^2) \,dy For revolution about a horizontal axis y=3y=3, the shell method requires integration with respect to yy. The shells are stacked from y=0y=0 to y=2y=2. The radius r(y)r(y) of a shell at height yy is its distance from the axis of revolution, so r(y)=3−yr(y) = 3-y. The height of the shell (which is its length in the x-direction) is given by h(y)=x=y2h(y) = x = y^2. The volume is therefore V=∫022πr(y)h(y) dy=∫022π(3−y)(y2) dyV = \int_0^2 2\pi r(y)h(y) \,dy = \int_0^2 2\pi (3-y)(y^2) \,dy.
  7. A solid is generated by rotating the region R bounded by y=x2y=x^2 and y=xy=\sqrt{x} about the line x=−1x=-1. What is the volume of the solid?
    Answer: 29π/3029\pi/30 We use the shell method. The curves intersect when x2=xx^2 = \sqrt{x}, giving x=0x = 0 and x=1x = 1. For 0≤x≤10 \leq x \leq 1, we have x≥x2\sqrt{x} \geq x^2. The radius of each shell is r(x)=x−(−1)=x+1r(x) = x - (-1) = x + 1 and the height is h(x)=x−x2h(x) = \sqrt{x} - x^2. The volume is V=∫012π(x+1)(x−x2)dx=2π∫01(x3/2−x3+x1/2−x2)dx=2π[25x5/2−x44+23x3/2−x33]01=2π(25−14+23−13)=2π(25−14+13)=2π⋅24−15+2060=29π30V = \int_0^1 2\pi(x+1)(\sqrt{x}-x^2)dx = 2\pi \int_0^1 (x^{3/2} - x^3 + x^{1/2} - x^2)dx = 2\pi[\frac{2}{5}x^{5/2} - \frac{x^4}{4} + \frac{2}{3}x^{3/2} - \frac{x^3}{3}]_0^1 = 2\pi(\frac{2}{5} - \frac{1}{4} + \frac{2}{3} - \frac{1}{3}) = 2\pi(\frac{2}{5} - \frac{1}{4} + \frac{1}{3}) = 2\pi \cdot \frac{24 - 15 + 20}{60} = \frac{29\pi}{30}.
  8. Let R be the region bounded by y=1/x2y=1/x^2, y=0y=0, x=1x=1, and x=2x=2. Let V1V_1 be the volume when R is revolved about the y-axis and V2V_2 be the volume when R is revolved about the x-axis. Which statement is true?
    Answer: V1=2πln⁡2V_1 = 2\pi \ln 2 and V2=7π/24V_2 = 7\pi/24 V1V_1 (revolve about y-axis): Use the shell method. V1=∫122πx(1/x2) dx=∫122π(1/x) dx=2π[ln⁡∣x∣]12=2π(ln⁡2−ln⁡1)=2πln⁡2V_1 = \int_1^2 2\pi x (1/x^2) \,dx = \int_1^2 2\pi (1/x) \,dx = 2\pi [\ln|x|]_1^2 = 2\pi(\ln 2 - \ln 1) = 2\pi \ln 2. V2V_2 (revolve about x-axis): Use the disk method. V2=∫12π(1/x2)2 dx=∫12πx−4 dx=π[x−3/(−3)]12=−π3[1/x3]12=−π3(1/8−1)=−π3(−7/8)=7π/24V_2 = \int_1^2 \pi (1/x^2)^2 \,dx = \int_1^2 \pi x^{-4} \,dx = \pi [x^{-3}/(-3)]_1^2 = -\frac{\pi}{3} [1/x^3]_1^2 = -\frac{\pi}{3} (1/8 - 1) = -\frac{\pi}{3} (-7/8) = 7\pi/24. Thus, V1=2πln⁡2V_1 = 2\pi \ln 2 and V2=7π/24V_2 = 7\pi/24.
  9. A solid is formed by revolving the region bounded by y=x2y = x^2, y=0y = 0, and x=2x = 2 around the line x=3x = 3. If we set up the shell method integral as V=2π∫abR(x)⋅H(x)dxV = 2\pi \int_a^b R(x) \cdot H(x) dx, what are the correct values of R(x)R(x) and H(x)H(x)?
    Answer: R(x)=3−xR(x) = 3 - x and H(x)=x2H(x) = x^2 When setting up the shell method for a solid of revolution, you need to identify two key components: the radius of each cylindrical shell and the height of each shell. For this problem, you're revolving the region bounded by y=x2y = x^2, y=0y = 0, and x=2x = 2 around the vertical line x=3x = 3. Since you're revolving around a vertical line, you'll integrate with respect to xx from x=0x = 0 to x=2x = 2. The radius R(x)R(x) is the horizontal distance from any point xx in your region to the axis of revolution x=3x = 3. Since your region spans from x=0x = 0 to x=2x = 2 (all to the left of x=3x = 3), this distance is 3−x3 - x. The height H(x)H(x) is the vertical extent of the region at any given xx-value, which runs from y=0y = 0 up to y=x2y = x^2, giving us H(x)=x2H(x) = x^2. Looking at the wrong answers: Choice A incorrectly uses R(x)=3+xR(x) = 3 + x, which would be the distance if you were measuring from x=−3x = -3 instead of to x=3x = 3. Choice B uses R(x)=x−3R(x) = x - 3, which gives negative values since x<3x < 3 in our region—radius must be positive. Choice D correctly identifies the radius but mistakenly uses H(x)=2−x2H(x) = 2 - x^2, which doesn't represent the height of our bounded region. Study tip: Always sketch the region and axis of revolution. For shell method radius, ask yourself: "How far is this strip from the axis?" The distance formula will guide you to the correct expression.
  10. The region bounded by y=x2y=x^2 and y=2xy=2x is revolved about the line x=3x=3. The volume of the resulting solid is given by V=∫022π(3−x)h(x) dxV = \int_0^2 2\pi (3-x)h(x) \,dx. What is the correct function for h(x)h(x)?
    Answer: h(x)=2x−x2h(x) = 2x - x^2 The problem uses the shell method, as indicated by the form of the integral. The term h(x)h(x) represents the height of the cylindrical shells. The region is bounded by y=2xy=2x (the upper curve) and y=x2y=x^2 (the lower curve) on the interval where they intersect, which is [0,2][0, 2]. The height of a vertical strip at a given xx is the difference between the upper function and the lower function. Therefore, h(x)=2x−x2h(x) = 2x - x^2.
  11. A solid is generated by revolving the region bounded by y=f(x)y=f(x) and y=g(x)y=g(x), where f(x)≥g(x)f(x) \ge g(x) on the interval [a,b][a,b], about the vertical line x=cx=c where c<ac < a. Which integral correctly represents the volume of this solid using the shell method?
    Answer: ∫ab2π(x−c)(f(x)−g(x)) dx\int_a^b 2\pi (x-c)(f(x)-g(x)) \,dx For the shell method with a vertical axis of revolution, we integrate with respect to xx. The height of a cylindrical shell at position xx is the difference between the upper and lower curves, h(x)=f(x)−g(x)h(x) = f(x)-g(x). The radius r(x)r(x) is the distance from the axis of revolution x=cx=c to the shell's position xx. Since c<a≤xc < a \le x, the distance is r(x)=x−cr(x) = x-c. The volume integral is V=∫ab2πr(x)h(x) dx=∫ab2π(x−c)(f(x)−g(x)) dxV = \int_a^b 2\pi r(x)h(x) \,dx = \int_a^b 2\pi (x-c)(f(x)-g(x)) \,dx.
  12. Consider the region bounded by y=exy = e^x, y=1y = 1, and x=ln⁡(3)x = \ln(3). When this region is revolved around the yy-axis using the shell method, which integral expression gives the correct volume?
    Answer: 2π∫0ln⁡(3)x(ex−1)dx2\pi \int_0^{\ln(3)} x(e^x - 1) dx When using the shell method to find volumes of revolution around the y-axis, you're essentially summing up cylindrical shells. Each shell has radius x, height given by the difference between functions, and thickness dx. First, let's visualize this region. The curve y=exy = e^x intersects y=1y = 1 when x=0x = 0 (since e0=1e^0 = 1). The vertical line x=ln⁡(3)x = \ln(3) gives us our right boundary, where y=eln⁡(3)=3y = e^{\ln(3)} = 3. So we have a region from x=0x = 0 to x=ln⁡(3)x = \ln(3), bounded above by y=exy = e^x and below by y=1y = 1. For the shell method around the y-axis, each vertical strip at position x becomes a cylindrical shell with: - Radius: x (distance from y-axis) - Height: ex−1e^x - 1 (top function minus bottom function) - Volume element: 2πx(ex−1)dx2\pi x(e^x - 1)dx Integrating from x=0x = 0 to x=ln⁡(3)x = \ln(3) gives us 2π∫0ln⁡(3)x(ex−1)dx2\pi \int_0^{\ln(3)} x(e^x - 1) dx, which is answer D. Answer A uses the washer method setup but incorrectly squares the radius term. Answer B also uses washer method thinking but with the wrong integrand. Answer C has the shell method format but incorrectly subtracts exe^x from 1, giving a negative height—remember that the exponential function is always above the horizontal line in this region. Study tip: Always sketch the region first and identify which function is on top. For shell method, the integrand should be radius × (outer function - inner function).
  13. The finite region enclosed by y=x2−4x+3y = x^2 - 4x + 3 and y=x−1y = x - 1 is revolved around the line y=−2y = -2. Using the shell method, what integral setup would be most efficient?
    Answer: 2π∫−20(y+2)[xright(y)−xleft(y)]dy2\pi \int_{-2}^0 (y + 2)[x_{right}(y) - x_{left}(y)] dy The curves intersect where x2−4x+3=x−1x^2 - 4x + 3 = x - 1, giving x2−5x+4=0x^2 - 5x + 4 = 0, so x=1x = 1 or x=4x = 4. Between these points, x−1>x2−4x+3x - 1 > x^2 - 4x + 3. Since we're revolving around the horizontal line y=−2y = -2, horizontal shells are more natural. For horizontal shells, the radius is y−(−2)=y+2y - (-2) = y + 2, and we integrate with respect to yy over the range of yy-values in the region. The yy-values range from the minimum of the parabola (at x=2x = 2: y=4−8+3=−1y = 4 - 8 + 3 = -1) to the intersection point values. Choice A uses vertical shells with wrong radius function. Choice C uses the wrong radius (should be distance to axis y=−2y = -2, not the parabola value plus 2). Choice D uses the line value plus 2 as radius, which is incorrect.
  14. A region in the first quadrant is bounded by x=y2x = y^2 and x=8−y2x = 8 - y^2. When revolved around the line x=−1x = -1, the volume using the shell method requires integration with respect to which variable and over what interval?
    Answer: Integration with respect to yy over [0,2][0, 2] The curves intersect where y2=8−y2y^2 = 8 - y^2, so 2y2=82y^2 = 8 and y=2y = 2 (in the first quadrant). For shell method around x=−1x = -1, we can use horizontal shells. Each shell has radius r=y−(−1)=y+1r = y - (-1) = y + 1 and height h=(8−y2)−y2=8−2y2h = (8 - y^2) - y^2 = 8 - 2y^2. We integrate with respect to yy from 00 to 22. Choice B would give vertical shells, but that's more complex since we'd need to solve for yy in terms of xx. Choice C uses wrong limits (should be 2, not 4). Choice D also uses wrong variable and limits.
  15. Let R be the region in the first quadrant bounded by y=4−x2y=4-x^2. Let VxV_x be the volume when R is revolved about the x-axis, and VyV_y be the volume when R is revolved about the y-axis. Which method is most efficient for calculating VyV_y, and what is the ratio Vy/VxV_y/V_x?
    Answer: Shell method is most efficient; ratio is 15/3215/32. VxV_x (revolve about x-axis): Use disk method. Limits are x=0x=0 to x=2x=2. Vx=∫02π(4−x2)2 dx=π∫02(16−8x2+x4) dx=π[16x−83x3+15x5]02=π(32−64/3+32/5)=256π/15V_x = \int_0^2 \pi (4-x^2)^2 \,dx = \pi \int_0^2 (16-8x^2+x^4) \,dx = \pi[16x - \frac{8}{3}x^3 + \frac{1}{5}x^5]_0^2 = \pi(32 - 64/3 + 32/5) = 256\pi/15. VyV_y (revolve about y-axis): Shell method is efficient. Limits x=0x=0 to x=2x=2. Radius r(x)=xr(x)=x, height h(x)=4−x2h(x)=4-x^2. Vy=∫022πx(4−x2) dx=2π[2x2−x4/4]02=2π(8−4)=8πV_y = \int_0^2 2\pi x(4-x^2) \,dx = 2\pi[2x^2 - x^4/4]_0^2 = 2\pi(8-4) = 8\pi. The washer method for VyV_y is also easy: Vy=∫04π(4−y)2 dy=π[4y−y2/2]04=π(16−8)=8πV_y = \int_0^4 \pi (\sqrt{4-y})^2 \,dy = \pi[4y-y^2/2]_0^4 = \pi(16-8)=8\pi. So both methods are efficient. The ratio is Vy/Vx=(8π)/(256π/15)=8⋅15/256=120/256=15/32V_y/V_x = (8\pi) / (256\pi/15) = 8 \cdot 15 / 256 = 120/256 = 15/32. Since both methods are efficient for VyV_y, we check the options. Both C and D have the correct ratio. But the shell method setup for VyV_y is arguably more direct from the function's given form y=f(x)y=f(x).
  16. The region bounded by y=sin⁡(x)y=\sin(x) and the x-axis from x=0x=0 to x=πx=\pi is revolved about the line x=−1x=-1. What is the volume of the resulting solid?
    Answer: 2π(π+2)2\pi(\pi+2) We use the shell method with respect to xx. The axis of revolution is x=−1x=-1. The radius of a shell at xx is the distance from xx to −1-1, which is r(x)=x−(−1)=x+1r(x) = x - (-1) = x+1. The height of the shell is h(x)=sin⁡(x)h(x) = \sin(x). The limits are from 00 to π\pi. The volume is V=∫0π2π(x+1)sin⁡(x) dx=2π∫0π(xsin⁡(x)+sin⁡(x)) dxV = \int_0^\pi 2\pi(x+1)\sin(x) \,dx = 2\pi \int_0^\pi (x\sin(x) + \sin(x)) \,dx. Using integration by parts, ∫xsin⁡(x) dx=−xcos⁡(x)+sin⁡(x)\int x\sin(x) \,dx = -x\cos(x) + \sin(x). The integral becomes 2π[−xcos⁡(x)+sin⁡(x)−cos⁡(x)]0π=2π[(−π(−1)+0−(−1))−(0+0−1)]=2π[(π+1)−(−1)]=2π(π+2)2\pi [-x\cos(x) + \sin(x) - \cos(x)]_0^\pi = 2\pi[(-\pi(-1) + 0 - (-1)) - (0+0-1)] = 2\pi[(\pi+1) - (-1)] = 2\pi(\pi+2).
  17. Consider the solid formed by revolving the region bounded by y=x2y=x^2 and y=4y=4 about the line x=3x=3. Let VSV_S be the integral for the volume using the shell method and VWV_W be the integral for the volume using the washer method. Which pair of integrals is correct?
    Answer: VS=∫−222π(3−x)(4−x2)dxV_S = \int_{-2}^2 2\pi (3-x)(4-x^2) dx and VW=∫04π((3+y)2−(3−y)2)dyV_W = \int_0^4 \pi ((3+\sqrt{y})^2 - (3-\sqrt{y})^2) dy Shell Method (integrate wrt xx): Axis is x=3x=3. The region spans x∈[−2,2]x \in [-2, 2]. Radius r(x)=3−xr(x)=3-x. Height h(x)=4−x2h(x)=4-x^2. So, VS=∫−222π(3−x)(4−x2)dxV_S = \int_{-2}^2 2\pi (3-x)(4-x^2) dx. Washer Method (integrate wrt yy): Axis is x=3x=3. The region spans y∈[0,4]y \in [0, 4]. The right boundary is x=yx=\sqrt{y} and left is x=−yx=-\sqrt{y}. The outer radius is the distance from x=3x=3 to the far curve x=−yx=-\sqrt{y}, so R(y)=3−(−y)=3+yR(y) = 3-(-\sqrt{y}) = 3+\sqrt{y}. The inner radius is the distance from x=3x=3 to the near curve x=yx=\sqrt{y}, so r(y)=3−yr(y) = 3-\sqrt{y}. Thus, VW=∫04π(R(y)2−r(y)2)dy=∫04π((3+y)2−(3−y)2)dyV_W = \int_0^4 \pi (R(y)^2 - r(y)^2) dy = \int_0^4 \pi ((3+\sqrt{y})^2 - (3-\sqrt{y})^2) dy.
  18. In the formula for the volume of a solid of revolution using the shell method, V=∫ab2πr(x)h(x) dxV = \int_a^b 2\pi r(x) h(x) \,dx, what does the expression 2πr(x)h(x)Δx2\pi r(x) h(x) \Delta x represent geometrically?
    Answer: The volume of a thin cylindrical shell with radius r(x)r(x), height h(x)h(x), and thickness Δx\Delta x. The shell method approximates the volume by summing the volumes of infinitesimally thin cylindrical shells. The term 2πr(x)2\pi r(x) is the circumference of the shell, h(x)h(x) is its height, and Δx\Delta x is its thickness. The product of circumference and height, 2πr(x)h(x)2\pi r(x) h(x), gives the lateral surface area of the cylinder. Multiplying this area by the thickness Δx\Delta x gives the approximate volume of that thin shell.
  19. Let R be the region in the first quadrant bounded by the graphs of y=x3y=x^3, the x-axis, and the line x=1x=1. Which integral represents the volume of the solid generated by revolving R about the line x=2x=2 using the shell method?
    Answer: V=∫012π(2−x)(x3) dxV = \int_0^1 2\pi (2-x)(x^3) \,dx Using the shell method for a vertical axis of revolution, the integral is with respect to xx. The region is bounded by x=0x=0 and x=1x=1. For a shell at a given xx, the height h(x)h(x) is given by the function y=x3y=x^3, so h(x)=x3h(x)=x^3. The radius r(x)r(x) is the distance from the axis of revolution x=2x=2 to the shell at xx, which is r(x)=2−xr(x)=2-x. The volume of a shell is 2πr(x)h(x)dx2\pi r(x)h(x)dx. Therefore, the total volume is given by the integral V=∫012π(2−x)(x3) dxV = \int_0^1 2\pi (2-x)(x^3) \,dx.
  20. Which integral represents the volume of the solid generated by revolving the region bounded by y=x2y=x^2 and y=xy=x about the line y=2y=2, using the shell method?
    Answer: ∫012π(2−y)(y−y) dy\int_0^1 2\pi(2-y)(\sqrt{y}-y) \,dy To use the shell method for revolution about a horizontal line (y=2y=2), we must integrate with respect to yy. First, express xx in terms of yy: x=yx=y and x=yx=\sqrt{y}. The region is bounded by y=0y=0 and y=1y=1. For a given yy, the right boundary is x=yx=\sqrt{y} and the left is x=yx=y. The height of a horizontal shell is h(y)=y−yh(y) = \sqrt{y}-y. The radius is the distance from the axis y=2y=2 to the shell, so r(y)=2−yr(y) = 2-y. The volume is V=∫012πr(y)h(y) dy=∫012π(2−y)(y−y) dyV = \int_0^1 2\pi r(y)h(y) \,dy = \int_0^1 2\pi(2-y)(\sqrt{y}-y) \,dy.

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