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PROOF 159

Prove.

The surface area of a sphere

In space.

A way to read this proof

First separate what is assumed from what is to be proved. At each step, ask which definition or earlier result permits the move. If it is unclear, return to that premise rather than skipping to the conclusion.

Definition D1

Write V(ρ) for the volume of the ball with center O and radius ρ, and S(ρ) for the area of the sphere bounding that ball.

Proof.

(1)S(ρ) is a fixed number for each ρ > 0.A1
(2)For 0 < ρ < σ, the set of all points whose distance from O is at least ρ and at most σ is called the shell of thickness σ − ρ.convention
(3)The ball of radius σ is divided without overlap into the ball of radius ρ and that shell, so the shell's volume is V(σ) − V(ρ)(2), A10

∎

Lemma L1

If t > 0, then S(r)·t ≤ V(r + t) − V(r) ≤ S(r + t)·t

Proof.

(1)The shell between the sphere of radius r and the sphere of radius r + t has thickness t, and its volume is V(r + t) − V(r).D1
(2)The volume of that shell is at least S(r)·t and at most S(r + t)·t.(1), A1, A2

∎

Lemma L2

If 0 < t < r, then S(r − t)·t ≤ V(r) − V(r − t) ≤ S(r)·t

Proof.

(1)r − t > 0, so the shell between the sphere of radius r − t and the sphere of radius r can be taken, and its thickness is t.assumption, D1
(2)The volume of that shell is V(r) − V(r − t).(1), D1
(3)Applying the squeeze with radius r − t and thickness t gives S(r − t)·t ≤ V(r) − V(r − t) ≤ S(r)·t(1), (2), A1, A2

∎

Lemma L3

V is differentiable and V′(r) = 4πr²

Proof.

(1)V(ρ) = ⁴⁄₃πρ³A3
(2)(ρ³)′ = 3ρ²A4
(3)V′(ρ) = ⁴⁄₃π × 3ρ² = 4πρ²(1), (2), A5, A11

∎

Theorem T

The area of a sphere of radius r is S(r) = 4πr²

Proof.

(1)For t > 0, dividing the left inequality of L1 by t gives S(r) ≤ (V(r + t) − V(r))/tL1, A9, A11
(2)As t → 0+ the right side tends to V′(r), and V′(r) = 4πr².A6, L3
(3)S(r) does not depend on t, so taking the limit gives S(r) ≤ 4πr²(1), (2), A7
(4)For 0 < t < r, dividing the right inequality of L2 by t gives (V(r) − V(r − t))/t ≤ S(r)L2, A9, A11
(5)Setting s = −t gives (V(r) − V(r − t))/t = (V(r + s) − V(r))/s, and t → 0+ is s → 0−, so this value tends to V′(r) = 4πr².A6, A11, L3, E
(6)Taking the limit gives 4πr² ≤ S(r)(4), (5), A7
(7)S(r) ≤ 4πr² and 4πr² ≤ S(r), so S(r) = 4πr²(3), (6), A8

∎

Remark

Can A2 be removed from this proof?

The computation that differentiates the volume, and the act of calling the derivative an area, are not on the same line. Separate which line is which.