Sphere has the minimum surface area?

AI Thread Summary
The discussion centers on proving that a sphere has the minimum surface area for a given volume, linked to the isoperimetric inequality in three dimensions. Participants suggest starting with a surface of revolution and applying the calculus of variations, specifically the Euler-Lagrange equation, to derive the necessary conditions for minimization. One user attempts to derive a differential equation from their variational formulation but encounters difficulties, indicating the complexity of the problem. They also mention the need to verify constants in their equations to solidify the proof. The conversation highlights the technical nature of the proof, emphasizing that it requires a deep understanding of calculus and variational principles.
persia7
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How do you prove that for a given volume, sphere has the minimum surface area?
 
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It is a standard problem in "Calculus of Variations" so you might also check that.
 
i tried to find proofs but i don't find please show me proofs
 
persia7 said:
i tried to find proofs but i don't find please show me proofs

How about first doing it for a surface of revolution, say for y(x) between -1 and 1. Then the surface is:

S=2\pi \int_{-1}^1 \sqrt{1+(y')^2}dx

and the volume of this surface of revolution is:

V=\pi \int_{-1}^1 y^2 dx
via discs.

Now, in the language of variation, we wish to minimize S while keeping V constant. The Euler condition for this problem is:

\frac{\partial H}{\partial y}-\frac{d}{dx}\frac{\partial H}{\partial y'}=0
with
H=V+\lambda S

Now, I've never solved this particular variational problem before ok, but if it were mine, I'd first see if I can get a circle out of Euler's equation thus showing me that a sphere has the minimum surface area for a given volume.
 
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jackmell said:
How about first doing it for a surface of revolution, say for y(x) between -1 and 1. Then the surface is:

S=2\pi \int_{-1}^1 \sqrt{1+(y')^2}dx

and the volume of this surface of revolution is:

V=\pi \int_{-1}^1 y^2 dx
via discs.

Now, in the language of variation, we wish to minimize S while keeping V constant. The Euler condition for this problem is:

\frac{\partial H}{\partial y}-\frac{d}{dx}\frac{\partial H}{\partial y'}=0
with
H=V+\lambda S

Now, I've never solved this particular variational problem before ok, but if it were mine, I'd first see if I can get a circle out of Euler's equation thus showing me that a sphere has the minimum surface area for a given volume.
can you show me a proof in internet?
 
thanks to all
 
persia7 said:
can you show me a proof in internet?

I worked with it a bit but ran into a DE I couldn't solve or else I had errors. But that's ok guys, don't tell me how to do it. I rag on others here about that: pretty soon you'll get to a problem that no one else on Earth can help you with and then you will have to go all by yourself so might as well get some practice. :)

Oh yeah, thanks guys for those references about isoperimetric inequality. All news to me. :)
 
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  • #10
Well, what do you expect? That is a very technical, difficult proof, involving, as I said before, "Calculus of Variations". Whole courses are taught on that subject! It isn't something you can expect to go over in an afternoon!
 
  • #11
I really was expecting the variational problem I set up to fall right through. Spent about an hour on it yesterday. I'm missing something because a get a really messy DE but maybe my approach is not the easiest variational formulation to use. Still though if the DE I derived at is correct, then I should be able to back-substitute the equation for a circle and get equality but when I do that I do not get equality so I got a problem.
 
  • #12
jackmell said:
How about first doing it for a surface of revolution, say for y(x) between -1 and 1. Then the surface is:

S=2\pi \int_{-1}^1 \sqrt{1+(y')^2}dx

Dang it! I'm missin' a y:

S=2\pi \int_{-1}^1 y \sqrt{1+(y')^2}dx


I think I need to review some things first . . .
 
  • #13
I get for the Euler equation:

1+(y')^2-yy''+\lambda y\left(1+(y')^2\right)^{3/2}=0
where \lambda is an arbitrary parameter.

Now, I'm going to cheat a little bit because I'm not good at this: I know the solution should be a circle, so when I substitute y(x)=\sqrt{1-x^2} into the left side of the DE above, in order for it to be zero, \lambda=-2. Therefore, we want to solve:

1+(y')^2-yy''-2y\left(1+(y')^2\right)^{3/2}=0

I started a thread in the DE forum because I needed help to solve it. It's here:

https://www.physicsforums.com/showthread.php?t=702671

Thanks to fzero and Jacquelin, we obtain:

\frac{dy}{dx}=\frac{\sqrt{y^2-(y^2-c_1)^2}}{y^2-c_1}

Now, just for the purpose of actually making progress with this problem albeit not the best way, I'm going to let c_1=0. Then we wish to solve:

\frac{dy}{dx}=\frac{\sqrt{1-y^2}}{y}

with the solution being:

y^2+(x+c_2)^2=1

Letting again c_2=0, we get the desired extremal: x^2+y^2=1.

All that remains to be done is to justify my particular values of the constants c_0, c_1,\lambda.

If someone can do this, I think we'd have a pretty decent proof of this theorem.

Also I forgot, this is only a necessary condition for a minimum. I think we would have to look into the second variation to prove this is a minimum.
 
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