Partial Surface Area of Oblate Spheroid?

hbchao
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Basically I have a horizontal tank with elliptical heads on each end. Given any liquid height, I would like to calculate the surface area which is in contact with the liquid.

The heads can be represented by a general oblate spheroid described by equation (x2 + y2)/a2 + z2/c2 = 1.

I can compute the partial surface area for z=XXX to YYY by taking the surface of revolution about the z-axis (ie for a vertical tank).

However how can I calculate the partial surface area for x=XXX to YYY?

I am not looking for a closed form equation, just something I can numerically integrate.
 
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Well, you could parametrize the oblate spheroid as follows:
x=a\sin\phi\cos\theta,y=a\sin\phi\sin\theta, z=c\cos\phi, 0\leq\phi\leq\frac{\pi}{2},0\leq\theta\leq{2\pi}
Note that these are tweaked spherical coordinates!

Thus, the surface \vec{S} can be represented as:
\vec{S}(\phi,\theta)=a\sin\phi\cos\theta\vec{i}+a\sin\phi\sin\theta\vec{j}+c\cos\phi\vec{k}

Local tangent vectors are then given by the partial derivatives of \vec{S}:
\vec{T}_{\phi}=\frac{\partial\vec{S}}{\partial\phi}
\vec{T}_{\theta}=\frac{\partial\vec{S}}{\partial\theta}

The local, infinitesemal area element is then the area of the parallellogram spanned by the infinitesemal tangent vectors \vec{T}_{\phi}d\phi,\vec{T}_{\theta}d\theta; and that equals ||\vec{T}_{\phi}\times\vec{T}_{\theta}||d\phi{d}\theta

We therefore get that the area A of one end can be calculated as:
A=\int_{0}^{\frac{\pi}{2}}\int_{0}^{2\pi}||\vec{T}_{\phi}\times\vec{T}_{\theta}||d\phi{d}\theta

which is some sort of elliptical integral, I think.
EDIT:
At least, it should be something like:
A=2ac\pi\int_{0}^{\frac{\pi}{2}}\sin\phi\sqrt{1+\frac{a^{2}-c^{2}}{c^{2}}\cos^{2}\phi}{d}\phi
 
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Hmm, on further thought, this should be exactly solvable!
Set u=\epsilon\cos\phi,\epsilon=\sqrt{\frac{a^{2}-c^{2}}{c^{2}}}
Thus, we get:
du=-\epsilon\sin\phi{d\phi}, or :
A=-\frac{ac\pi}{\epsilon}\int_{\epsilon}^{0}\sqrt{1+u^{2}}du=\frac{ac\pi}{\epsilon}\int^{\epsilon}_{0}\sqrt{1+u^{2}}du
Setting u=Sinh(v), and we readily integrate the expression!
 
Thanks for the reply...however it has been many years since my high school/college days and I'm having a bit of a hard time following the transformation...

If the liquid level in the tank is X, how would I go about determining the limits of integration?
 
hbchao said:
Thanks for the reply...however it has been many years since my high school/college days and I'm having a bit of a hard time following the transformation...

If the liquid level in the tank is X, how would I go about determining the limits of integration?

Well, one half of the oblate spheroid should, if I did this correctly (I forgot a factor of 2 from my next to last post), be:
A=\pi(ac\frac{Sinh^{-1}\epsilon}{\epsilon}+a^{2}), \epsilon=\sqrt{\frac{a^{2}-c^{2}}{c^{2}}},a\geq{c})
Note that this yields half the sphere's surface area when a=c.

I'm sure you can find out the rest of your answer by yourself.
 
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