W9.3.8 volume by rotation

In summary: Using the shell method:dV=2\pi rh\,dyr=y-1h=x-2=2\left(2y^{-\frac{1}{3}}-1\right)Hence:dV=4\pi (y-1)\left(2y^{-\frac{1}{3}}-1\right)\,dyV=4\pi\int_1^8 2y^{\frac{2}{3}}-y-2y^{-\frac{1}{3}}+1\,dy=20\pi
  • #1
karush
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http://mathhelpboards.com/attachment.php?attachmentid=5579&stc=1
W9.3.8
Let $S$ be the region of the xy-plane bounded above by the curve $x^{3} y = 64$
below by the line $y = 1$, on the left by the line $x = 2$,
and on the right by the line $x = 4$. Find the volume of the solid obtained by rotating S around
(a) the -axis,
(b) the line $y = 1$,
(c) the y-axis,
(d) the line $x = 2$ . Not sure how to set this up

Was going to use shell method which basically is

$$2\pi\int_{a}^{b}y f\left(y\right) \,dy $$
 
Last edited:
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  • #2
karush said:
W9.3.8
Let $S$ be the region of the xy-plane bounded above by the curve $x^{3} y = 64$
below by the line $y = 1$, on the left by the line $x = 2$,
and on the right by the line $x = 4$. Find the volume of the solid obtained by rotating S around
(a) the -axis,
(b) the line $y = 1$,
(c) the y-axis,
(d) the line $x = 2$ . Not sure how to set this up

Was going to use shell method which basically is

$$2\pi\int_{a}^{b}y f\left(y\right) \,dy $$

Since you are rotating around the x axis, approximate the area under the curve with rectangles of width $\displaystyle \begin{align*} y = \frac{64}{x^3} \end{align*}$ and very small length $\displaystyle \begin{align*} \Delta x \end{align*}$. Then the volume can be approximated by rotating each of these rectangles around the x axis, giving small cylinders of radius $\displaystyle \begin{align*} y = \frac{64}{x^3} \end{align*}$ and height $\displaystyle \begin{align*} \Delta x \end{align*}$. Then the volume of each small cylinder is $\displaystyle \begin{align*} \pi \, y^2 \, \Delta x \end{align*}$ and the total volume is then approximately $\displaystyle \begin{align*} \sum{ \pi \, y^2 \, \Delta x } \end{align*}$.

As we increase the number of rectangles (to infinity) by making $\displaystyle \begin{align*} \Delta x \end{align*}$ smaller (to 0), the approximation becomes exact and the sum converges on an integral. Thus the volume generated by rotating $\displaystyle \begin{align*} y = \frac{64}{x^3} \end{align*}$ between x = 2 and x = 4 is

$\displaystyle \begin{align*} V &= \int_2^4{ \pi \, \left( \frac{64}{x^3} \right) ^2 \, \mathrm{d}x } \\ &= 4096\,\pi \int_2^4{ x^{-6}\,\mathrm{d}x } \\ &= 4096\,\pi \, \left[ \frac{x^{-5}}{-5} \right]_2^4 \\ &= -\frac{4096}{5}\,\pi\,\left[ \frac{1}{x^5} \right]_2^4 \\ &= -\frac{4096}{5} \, \pi \, \left( \frac{1}{4^5} - \frac{1}{2^5} \right) \\ &= -\frac{4096}{5}\,\pi \, \left( -\frac{31}{1024} \right) \\ &= \frac{124}{5}\,\pi \end{align*}$

Now we have to think about what would happen if we remove the volume of the cylinder that is formed from there being a boundary at y = 1 as well...
 
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  • #3
Thanks for all the steps
I'm going to do more volume problems today till I get a good handle on it😎😎😎
 
  • #4
b. About $y=1$

$$y_1=\frac{64}{{x}^{3}}$$

$$\pi\int_{2}^{4}\left(y_1-1\right)^2 \,dy = \frac{74 \pi}{5 }$$
 
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  • #5
About y-axis

$$\pi\int_{1}^{8}\left(x_1(y)^2 -2^2 \right) \,dy = 20 \pi$$

About x=2 ?
 
  • #6
karush said:
b. About $y=1$

$$y_1=\frac{64}{{x}^{3}}$$

$$\pi\int_{2}^{4}\left(y_1-1\right)^2 \,dy = \frac{74 \pi}{5 }$$

Let's check that using the shell method:

\(\displaystyle dV=2\pi rh\,dy\)

\(\displaystyle r=y-1\)

\(\displaystyle h=x-2=2\left(2y^{-\frac{1}{3}}-1\right)\)

And so we have:

\(\displaystyle dV=4\pi (y-1)\left(2y^{-\frac{1}{3}}-1\right)\,dy\)

\(\displaystyle V=4\pi\int_1^8 2y^{\frac{2}{3}}-y-2y^{-\frac{1}{3}}+1\,dy=\frac{74\pi}{5}\checkmark\)
 
  • #7
Well that helped a lot to understand the shell mdthod😄😄
 
  • #8
karush said:
About y-axis

$$\pi\int_{1}^{8}\left(x_1(y)^2 -2^2 \right) \,dy = 20 \pi$$

About x=2 ?

About the $y$-axis:

Washer method:

\(\displaystyle dV=\pi\left(R^2-r^2\right)\,dy\)

\(\displaystyle R=x\)

\(\displaystyle r=2\)

Hence:

\(\displaystyle dV=\pi\left(x^2-2^2\right)\,dy=4\pi\left(4y^{-\frac{2}{3}}-1\right)\,dy\)

And so we have:

\(\displaystyle V=4\pi\int_1^8 4y^{-\frac{2}{3}}-1\,dy=20\pi\)

Shell method:

\(\displaystyle dV=2\pi rh\,dx\)

\(\displaystyle r=x\)

\(\displaystyle h=y-1=64x^{-3}-1\)

Hence:

\(\displaystyle V=2\pi\int_2^4 64x^{-2}-x\,dx=20\pi\)

Can you give $x=2$ as the axis of revolution a try now? Whichever way you do it, I will do it the other way as a check. :)
 
  • #9
$y_1=\frac{64}{{x}^{3}}$

$x-2=r$

$$2 \pi \int_{2 }^{4 }r\left(y_1-1\right) \,dx=4\pi$$
 
  • #10
karush said:
$y_1=\frac{64}{{x}^{3}}$

$x-2=r$

$$2 \pi \int_{2 }^{4 }r\left(y_1-1\right) \,dx=4\pi$$

Using the disk method:

\(\displaystyle dV=\pi r^2\,dy\)

\(\displaystyle r=x-2=2\left(2y^{-\frac{1}{3}}-1\right)\)

Hence:

\(\displaystyle V=4\pi\int_1^8 4y^{-\frac{2}{3}}-4y^{-\frac{1}{3}}+1\,dy=4\pi\)
 

What is "W9.3.8 volume by rotation"?

W9.3.8 volume by rotation is a mathematical concept that involves finding the volume of a three-dimensional object by rotating a two-dimensional shape around an axis.

How is "W9.3.8 volume by rotation" different from regular volume?

Regular volume is calculated by finding the amount of space occupied by a three-dimensional object, while W9.3.8 volume by rotation involves calculating the volume of an object by rotating a two-dimensional shape around an axis.

What types of objects can be measured using "W9.3.8 volume by rotation"?

Any three-dimensional object that can be formed by rotating a two-dimensional shape around an axis can be measured using W9.3.8 volume by rotation. This includes objects such as cylinders, cones, and spheres.

How is "W9.3.8 volume by rotation" used in real-life applications?

W9.3.8 volume by rotation is commonly used in engineering and construction to calculate the volume of objects such as pipes, tanks, and containers. It is also used in fields such as physics and chemistry to measure the volume of irregularly shaped objects.

What is the formula for calculating "W9.3.8 volume by rotation"?

The formula for calculating W9.3.8 volume by rotation is V = π∫(f(x))^2dx, where V is the volume, π is the mathematical constant pi, ∫ represents an integral, f(x) is the function that describes the shape being rotated, and dx represents an infinitesimal change in the distance along the axis of rotation.

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