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2008年7月29日 星期二

循環論證 (II) : 圓周公式

Continue from 循環論證 (I) : 圓周公式



There should be no controversy before the integral arises,

let's verify each steps carefully starting from the arc length.


\int_{0}^{r}\sqrt{1+\frac{dy}{dx}^2}\,dx

The arc length formula itself is correct.

Its proof is based on Mean Value Theorem and Riemann Sum.


Here, what we need to verify is the differentiability of \inline y=\sqrt{r^2-x^2} on the interval \inline \left(0,r\right) and the continuity on \inline \left[0,r\right].

Both of them are clear except the continuity at the end-point 0.

But, since we are considering the first quadrant only, the existence of one hand limit is enough.


For the symmetry part, there should be no problem.

{If you really think about it, just consider the properties of the odd function and even function}


Afterwards, the simplification of integral is obviously correct.

Then, we investigate the computation of integral.

L=4r\left[\sin^{-1} \frac{x}{r} \right]_{0}^{r}  \cdots (1)

L=4r\left[\frac{\pi}{2}-0\right]=2\pi r \cdots (2)


As I mentioned in the first part, there must be a flaw in the proof, so the flaw should arise in the computation part.


Before we proceed, let's recall the following high-school definitions:



\inline \pi is defined as the common ratio of circumference to diameter of any circle.


Radian is defined as the ratio of arc length to the radius of a circle, in particular, it is the arc length of the unit circle.


\inline \left(\sin x,\cos x\right) is defined as the point lying on the unit circle making an angle x (in radian) with the x-axis.


\inline \sin^{-1} x is then defined as the inverse mapping on the right half of the unit circle


Let's consider the second equation first, as this is easier to explain.

Here, we use the common sense that \inline \sin^{-1}1=\tfrac{\pi}{2} and \inline\sin^{-1}0=0 , but why!?

somehow we know \inline \sin\tfrac{\pi}{2}=1

(we must rely on the fact that \inline \pi is the ratio)

So, we found that the second one contains flaw.

However, this does not mean that the first one contains no circular reasoning.
For those who knows a little bit of analysis,

For the first equation, we used Fundamental theorem of Calculus, which itself require the function \inline \sin^{-1}x to be integrable, being the inverse function of \inline \sin x, it is continuous, and hence integrable.

To show that \inline \sin x is a continuous function, from epsilon-delta definition, the inequality \inline \left|\sin x - \sin y\right| \leq \left|x - y\right| must be involved, which is often proved using geometric argument

2008年3月17日 星期一

循環論證 (I) --- 圓周公式


這是 ami 第一篇在手記放的貼子,題目早於一個月前決定,今天比較空閒終於有機會貼上來。

在教會教一班中學生數學時,其中有一人 X 問道以下一道問題:


X : 給出一個圓形,圓周為 r,圓面積的公式 \pi r^2能夠運用積分的方法來證明。

X : 那麼,請問圓形的圓周 2\pi r 可否運用類近的積分算式去「證明」呢?


附註:

X 提問時,特別強調證明一詞。

\pi定義熟悉的讀者,應該明白背後的原因吧。


與此同時,有另一位曾經修讀純數的人給出以下證明:


L 為給出圓形的圓周,設圓的圓心為 \left(0,0\right),所以圓的方程為x^2+y^2=r^2


Let L be the circumference of the given circle, suppose the circle center at origin, so the equation of circle is x^2+y^2=r^2.


考慮圓形在第一象限:


Consider the first quadrant:


y=\sqrt{r^2-x^2}


由弧長公式及對稱性可知 :


By arc length integral and symmetry:


L=4\int_{0}^{r}\sqrt{1+\left(\frac{dy}{dx}\right)^2}\,dx


約簡後得出:

After simplification :


L=4r\int_{0}^{r}\frac{1}{\sqrt{r^2-x^2}}\,dx


所以

Therefore :


L=4r\left[\sin^{-1}\frac{x}{r}\right]_{0}^{r}=4r\left[\frac{\pi}{2}-0\right]=2\pi r


究竟在「證明」中有什麼錯誤呢?


由於時間所限,留待下一篇才解答吧。




For reference:
Definition of Pi
Arc length forumla