MHB The volume of the solid generated by the revolution

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The discussion centers on finding the volume of the solid generated by revolving the curve defined by the equation y^2(2a - x) = x^3 around its asymptote, the line x = 2a. Participants agree that the shell method is the most practical approach due to the ease of solving for y compared to x. The volume is calculated using the formula for the volume of an arbitrary shell and integrating over the appropriate limits. The final volume is determined to be V = 2π^2a^3. This method effectively demonstrates the application of calculus in determining volumes of revolution.
ksananthu
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find the volume of the solid generated by the revolution of the curve
$y^2 (2 a - x) = x^3$ about its asymptote.
 
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Re: the volume of the solid generated by the revolution

Have you identified the axis of revolution, i.e., the asymptote, and have you observed which method of computing the solid is the most practical and why?
 
Re: the volume of the solid generated by the revolution

i think shell method is best
 
Re: the volume of the solid generated by the revolution

ksananthu said:
i think shell method is best

So do I...can you explain why?
 
Since more than 24 hours has gone by since the last response by the OP, I am going to post the solution while it is still on my mind.

First, I plotted the implicit curve, letting $a=1$:

View attachment 1023

Now, it is fairly easy to see that the domain of the implicit function is $[0,2a)$, if we write it in the form:

[math]y^2=\frac{x^3}{2a-x}\ge0[/math]

We also see that the axis of rotation, i.e., the asymptote is the line $x=2a$.

We should observe that the shell method is more practical since we can solve for $y$ but not for $x$, at least not easily. Also, the disk method would generate an improper integral, so we would need to determine if it converges. So, let's proceed with the shell method. The volume of an arbitrary shell is:

[math]dV=2\pi rh\,dx[/math]

where:

[math]r=2a-x[/math]

[math]h=2\sqrt{\frac{x^3}{2a-x}}[/math]

Since $x$ is non-negative in the domain, we may write:

[math]h=2x\sqrt{\frac{x}{2a-x}}[/math]

and so we find:

[math]dV=4\pi(2a-x)x\sqrt{\frac{x}{2a-x}}\,dx=4\pi x\sqrt{x(2a-x)}\,dx[/math]

Thus, summation of the shells gives us the volume:

[math]V=4\pi\int_0^{2a} x\sqrt{x(2a-x)}\,dx[/math]

Completing the square under the radical, we obtain:

[math]V=4\pi\int_0^{2a} x\sqrt{a^2-(x-a)^2}\,dx[/math]

Now, if we let:

[math]x-a=a\sin(\theta)\,\therefore\,dx=a\cos(\theta)[/math]

we obtain:

[math]V=4\pi a^3\int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} (1+\sin(\theta))\cos^2(\theta)\,d\theta= 4\pi a^3\left(\int_{-\frac{\pi}{2}}^{\frac{\pi}{2}}\cos^2(\theta)\,d \theta+ \int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} \cos^2(\theta)\sin(\theta)\,d\theta \right)[/math]

For the first integral, using a double-angle identity for cosine, we may write:

[math]\int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} \cos^2(\theta)\,d\theta= \frac{1}{2}\int_{-\frac{\pi}{2}}^{\frac{\pi}{2}}1+ \cos(2\theta)\,d\theta= \frac{1}{2}\left([\theta]_{-\frac{\pi}{2}}^{\frac{\pi}{2}}+ \frac{1}{2}[\sin(2\theta)]_{-\frac{\pi}{2}}^{\frac{\pi}{2}} \right)= \frac{\pi}{2}[/math]

For the second integral, using the odd function rule, we may write:

[math]\int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} \cos^2(\theta)\sin(\theta)\,d\theta=0[/math]

And so we have:

[math]V=4\pi a^3\left(\frac{\pi}{2} \right)=2\pi^2a^3[/math]
 

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Thank you.
i tried same way and I got the answer !
 
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