How is this formula for the surface derived?

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The discussion centers on the derivation of the formula for the surface area of a sphere and the relevance of the sphere's wall thickness, t. It is established that the surface area of a sphere is given by 4πr², but the area of the cut surface is more accurately described by the formula 2πrt - πt² when considering thickness. The approximation holds true when t is significantly smaller than r, allowing the quadratic term to be negligible. Participants also confirm that for a sphere with an infinitely thin wall, the inner and outer surface areas can be considered equal, although slight discrepancies arise in calculus when taking limits. Overall, the discussion clarifies the relationship between thickness and surface area in spherical geometry.
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Homework Statement
This is not a homework problem. I am struggling with a formula for the inner area of semicircular sphere, mentioned in a book
Relevant Equations
Area = ## 2 \pi . r . t ##

where, r is the radius of the sphere and t is the thickness of its wall.
The formula is shown at the bootom of picture 1.
The pages shown in the pictures are from an engineering book. I am not sure how the thickness of sphere plays a role in the inner surface of the sphere. I know that the surface area of sphere is ##4 \pi r^2 ## .

Picture 2 shows how that formula plays a role in understanding the stress expereinced by the sphere. I am not sure how the thickness, t, of the sphere wall is relevant here.

Thanks
 

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The ##2\pi rt## is the area of the cut surface, according to the text. A ring with radius ##r## and width ##t##.
 
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musicgold said:
I am not sure how the thickness, t, of the sphere wall is relevant here.
As @BvU already said, they're talking about the area of the cut surface.

Furthermore, the area they give is only approximately correct, and is assuming that the thickness t is small in comparison to the radius r.

The actual area of the cut surface is ##\pi r^2 - \pi(r - t)^2 = \pi(r^2 - r^2 - 2rt + t^2) = 2\pi rt - \pi t^2##
If ##t << r##, the term ##\pi t^2## won't subtract much from the first term.
 
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Mark44 said:
Furthermore, the area they give is only approximately correct, and is assuming that the thickness t is small in comparison to the radius r.
The actual area of the cut surface is ##\pi r^2 - \pi(r - t)^2 = \pi(r^2 - r^2 - 2rt + t^2) = 2\pi rt - \pi t^2##
If ##t << r##, the term ##\pi t^2## won't subtract much from the first term.

Oh, now I get it! Thanks.

Also, I have a a follow up question.

Is it fair to assume that for a sphere with an infinitely thin wall, the inner surface area is equal to the outer surface area?
 
musicgold said:
Is it fair to assume that for a sphere with an infinitely thin wall, the inner surface area is equal to the outer surface area?

Yes.

Although if you're taking the "infinitesimal limit" as in some calculus proof, it won't perfectly cancel and you'll end up with a little differential term which goes to zero in the case that is is literally zero thickness.
 
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The outer and inner surface areas of a shell of outer radius ##R## and inner radius ##(R-t)## are$$A_{outer}=4\pi R^2~;~~~A_{inner}=4\pi (R-t)^2=A_{outer}\left(1-\frac{2t}{R}+\frac{t^2}{R^2}\right).$$ The expression for ##A_{inner}## is exact. You can ignore the quadratic term or both quadratic and linear terms depending on how small the ratio ##t/R## is relative to ##1##.
 
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