Sphere has the minimum surface area?

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SUMMARY

The discussion centers on proving that a sphere has the minimum surface area for a given volume, a concept rooted in the isoperimetric inequality in three dimensions. The participants explore the variational problem using the Euler-Lagrange equation, specifically focusing on the surface of revolution defined by the function y(x) between -1 and 1. Key equations include the surface area S and volume V expressed through integrals. The conversation highlights the complexity of the proof, emphasizing the need for a deeper understanding of Calculus of Variations and differential equations.

PREREQUISITES
  • Understanding of the isoperimetric inequality in three dimensions
  • Familiarity with Calculus of Variations
  • Knowledge of Euler-Lagrange equations
  • Basic skills in solving differential equations
NEXT STEPS
  • Study the isoperimetric inequality proofs available at Cornell Math and Stanford University
  • Learn about the Euler-Lagrange equation and its applications in variational problems
  • Explore advanced techniques in solving differential equations related to variational calculus
  • Review the principles of surface area and volume calculations for surfaces of revolution
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Mathematicians, physics students, and anyone interested in advanced calculus, particularly those studying variational principles and geometric optimization.

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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