Sphere has the minimum surface area?

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Discussion Overview

The discussion centers around the question of how to prove that a sphere has the minimum surface area for a given volume. It touches on concepts from calculus, particularly the isoperimetric inequality and the calculus of variations, and involves both theoretical and mathematical reasoning.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • Some participants suggest that the problem is a special case of the isoperimetric inequality in three dimensions.
  • Others mention that it is a standard problem in the calculus of variations and recommend checking relevant literature.
  • Several participants express difficulty in finding proofs and request assistance or references.
  • One participant proposes starting with a surface of revolution and sets up the equations for surface area and volume, indicating a desire to minimize surface area while keeping volume constant.
  • A participant shares their approach using the Euler condition for variational problems but notes challenges in solving the resulting differential equation.
  • Another participant acknowledges the technical difficulty of the proof and emphasizes that it requires a deep understanding of calculus of variations.
  • One participant discusses their progress on the Euler equation and mentions needing help with solving it, while also noting that their approach may not be the easiest formulation.
  • Another participant expresses frustration with deriving a messy differential equation and questions their approach.
  • One participant provides links to external resources for proofs related to the isoperimetric inequality.

Areas of Agreement / Disagreement

Participants generally agree that the problem is complex and involves advanced mathematical concepts, but there is no consensus on a specific proof or approach. Multiple competing views and methods are presented, and the discussion remains unresolved.

Contextual Notes

Participants mention various assumptions and approaches, including the need for specific conditions to be met in their formulations. There are unresolved mathematical steps and challenges in deriving the necessary equations for the proof.

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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