I need to find a formula for the surface area of a solid of revolution rotated around the $y$-axis. The curve is $f(x)=x^2$ on $[0,1]$. However, my answer must be in terms of $f$, not $f^{-1}$.
[Math] Surface area of revolution about $y$-axis in terms of $f(x)$
calculusintegrationsolid-geometry
Related Solutions
Hint: Try to substituted $3y=t$ first and then use the second of the following fact:
Theorem: The integral
$$\int x^m(a+bx^n)^pdx$$
can be reduced if $m,n,p$ are rational numbers, to the integral of a rational function, and can thus be expressed in terms of elementary functions if:
$1.$ $p$ is an integer( $p>0$ use the Newton's binomial theorem and when $p<0$ then $x=t^k$ which $\text{lcm}(n,m)$).
$2.$ $\dfrac{m+1}{n}$ is an integer. So set $a+bx^n=t^{\alpha}$ wherein $\alpha$ is the denominator of $p$.
$3.$ $\dfrac{m+1}{n}+p$ is an integer.
Here we have $p=1/2,n=-4/3,m=1/3$
[Math] How to find the surface area of revolution of an ellipsoid from ellipse rotating about y-axis
I'm going to assume that the ellipse has the equation
$$\frac{x^2}{a^2} + \frac{y^2}{b^2} = 1$$
since that's the more standard assumption. Yours has $a$ and $b$ reversed and I'm not sure if you meant it that way or if that was a typo on your part (I think it was a typo since your expression for the eccentricity matches the standard one). I'll also assume $a \ge b$. The case $b \ge a$ is handled similarly.
Now imagine that you rotate the ellipse around its long axis, that is, around the $x$ axis, and focus your attention on the strip that results from rotating a small arc of the ellipse, located at $(x,y)$ before the rotation. That elliptical arc has a length $ds$ that depends on its location, so it's a function of $(x,y)$. In fact, it's not hard to show that that arc-length is given by
$$ds = dx\,\sqrt{1 + (\frac{dy}{dx})^2}$$
Anyway, the strip resulting from the rotation of that little elliptical arc has a circular shape and, therefore, an area approximately equal to
$$dA = 2\pi\,\mbox{radius} \times ds$$
and you can see from the figure that the radius is just $y$, so
$$dA = 2\pi\,y\,ds$$
Now, given the equation at the top, we find
$$\frac{2x\,dx}{a^2} + \frac{2y\,dy}{b^2} = 0$$
so
$$\frac{dy}{dx} = -\frac{b^2}{a^2}\,\frac{x}{y}$$
and
$$ds = \frac{1}{a^2}\,\frac{dx}{y}\,\sqrt{b^4x^2 + a^4y^2}$$
As promised, $ds$ depends on $(x,y)$. Putting all of the above together, we find
$$dA = dx\,\frac{2\pi}{a^2}\,\sqrt{b^4x^2 + a^4y^2}$$
The area of the entire surface of revolution is then twice the integral of the above expression, from $x=0$ to $x=a$. Twice because we're integrating over only half the ellipse:
$$A = \frac{4\pi}{a^2}\int_{x\,=\,0}^{x\,=\,a} \sqrt{b^4x^2 + a^4y^2}\,dx$$
We still need to eliminate $y$, but that's easy. From the equation at the top, we find
$$y^2 = b^2 - \frac{b^2}{a^2}\,x^2$$
and then:
$$A = 4\pi\,\frac{b}{a}\int_{x\,=\,0}^{x\,=\,a} \sqrt{a^2 - (\frac{a^2 - b^2}{a^2})\,x^2}\,dx$$
The quantity
$$\frac{a^2 - b^2}{a^2}$$
is none other than the ellipse's eccentricity $\varepsilon$. So, finally, we have
$$A = 4\pi\,\frac{b}{a}\int_{x\,=\,0}^{x\,=\,a} \sqrt{a^2 - \varepsilon^2x^2}\,dx$$
Now use the parametrisation $x = a\,\sin\theta$ (Why $\sin$ instead of $\cos$? Because it makes the math easier down below. Shouldn't it be $\cos$, though? Not necessarily. Note that $x$ is now a dummy integration variable and we can choose any substitution we want) to get
$$A = 4\pi\,ab\,\int_{\theta\,=\,0}^{\theta\,=\,\pi/2} \sqrt{1 - \varepsilon^2\sin^2\theta}\,\cos\theta\,d\theta$$
Next set $\sin\phi = \varepsilon\sin\theta$ so $\cos\phi\,d\phi = \varepsilon\cos\theta\,d\theta$ and
$$A = 4\pi\,\frac{ab}{\varepsilon}\,\int\cos^2\phi\,d\phi$$
(I omitted the integration limits but will get back to them below)
To integrate $\cos^2\phi$, we can use the fact that $\cos(2\phi) = \cos^2\phi - \sin^2\phi = 2\cos^2\phi - 1$. Thus,
$$\cos^2\phi = \frac{1 + \cos(2\phi)}{2}$$
and
$$\int\cos^2\phi\,d\phi = \int\frac{1 + \cos(2\phi)}{2}\,d\phi = \frac{\phi}{2} + \frac{\sin(2\phi)}{4} $$
Now back to the integration limits. Note that $\theta = 0$ implies $\sin\phi = 0$, thus $\phi = 0$, and $\theta = \pi/2$ implies $\sin\phi = \varepsilon$, that is, $\phi = \arcsin(\varepsilon)$. Note also that $0 \le \varepsilon \le 1$ since $a \ge b$.
So then we get
$$A = 2\pi\,\frac{ab}{\varepsilon}\,(\phi + \frac{\sin(2\phi)}{2})\,\big|_{0}^{\arcsin(\varepsilon)} = 2\pi\,\frac{ab}{\varepsilon}\,\big[\,\arcsin(\varepsilon) + \frac{\sin(2\arcsin(\varepsilon))}{2}\,\big] $$ Then, using $\sin(2\phi) = 2\sin\phi\cos\phi$, we find
$$A = 2\pi\,\frac{ab}{\varepsilon}\,\big(\,\arcsin(\varepsilon) + \varepsilon\sqrt{1-\varepsilon^2}\,\big) $$
Finally, using the definition of the eccentricity, we get
$$A = 2\pi\,\frac{ab}{\varepsilon}\,\big(\,\arcsin(\varepsilon) + \varepsilon\,\frac{b}{a}\,\big) = 2\pi\,b^2\,\big(1 + \frac{a}{b}\,\frac{\arcsin(\varepsilon)}{\varepsilon} \,\big) $$
which is the expression you wanted to prove.
Best Answer
The only thing that changes when you revolve the curve about the $y$-axis instead of the $x$-axis is the expression for the radius of revolution. When you revolve it about the $x$-axis, the radius of revolution at a particular value of $x$ is $|f(x)|$, the distance from the curve to the $x$-axis; when you revolve it about the $y$-axis, the radius is $|x|$, the distance from the curve to the $y$-axis.
The element $dA$ of surface area at a given $x\in[0,1]$ is still $dA=2\pi x\,ds$, since the radius of revolution about the $y$-axis is simply $x$ in this case. From studying arc length you know that
$$ds=\sqrt{1+\left(\frac{dy}{dx}\right)^2}\,dx=\sqrt{1+\big(f\,'(x)\big)^2}\;,$$ so
$$dA=2\pi x\sqrt{1+\left(\frac{dy}{dx}\right)^2}\,dx=2\pi x\sqrt{1+\left(f\,'(x)\right)^2}\,dx\;;$$
now just integrate $dA$ over the appropriate range of values of $x$.