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Can anyone please show me , using simple integration, how the area of a circle turns out to be (Pi)r^2 ? I've tried many ways and sometimes I end up with 2(Pi)r or completely irrelevant answers ... :S
Thanks
Last edited by Chemist (2005-12-19 09:21:07)
"Fundamentally one will never be able to renounce abstraction."
Werner Heisenberg
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Start with x²+y² = r²
Then integrate just the top half, which is y = √( r²-x² )
I think it gets a little complicated after that.
"The physicists defer only to mathematicians, and the mathematicians defer only to God ..." - Leon M. Lederman
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I can do it with polar co-ordinates.
For a circle, the magnitude doesn't depend on θ, so the equation would just be r=a, where a is a constant and is also the radius of the circle.
It's a given formula that the area of a region using polar co-ordinates is (0,2π)∫1/2r² dθ. [That's meant to mean integrating between 0 and 2π, but I'm bad at LaTeX]
So, using r=a, that is (0,2π)∫1/2a²dθ
As this doesn't involve θ, integrating merely multiplies the whole thing by θ.
Area = [1/2a²θ](0,2π) = [1/2a²*2π] - [1/2a²*0] = πa².
Why did the vector cross the road?
It wanted to be normal.
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Found a nice page about it here
"The physicists defer only to mathematicians, and the mathematicians defer only to God ..." - Leon M. Lederman
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Then integrate just the top half, which is y = √( r²-x² )
I think it gets a little complicated after that.
Indeed I tried that, and yes the poblem is with the integration.
mathsyperson, your method is good, but since I'm doing this from scratch, just why is the area (0,2π)∫1/2r² dθ ?
Thank your both for your time.
"Fundamentally one will never be able to renounce abstraction."
Werner Heisenberg
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Ah just what I need, thanks man.
"Fundamentally one will never be able to renounce abstraction."
Werner Heisenberg
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I didn't go to those web sites, so here is maybe another way.
Allow the knowledge of a circumference being around 3 times the diameter (2π r)
If you don't approve of knowing this, then don't read on.
Imagine many concentric circles around the origin varying from really small to
a radius of one or r, if you want the general case. I'll use 1 for largest r.
Now the concentric circles are evenly spaced apart, and adding up their circumferences
times the distance between the circles should be about right.
Hence
igloo myrtilles fourmis
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Integrate 2π r dr to get π r² ... ?
It might just work ...
... nah, too easy
"The physicists defer only to mathematicians, and the mathematicians defer only to God ..." - Leon M. Lederman
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That works with spheres too.
∫ 4πr²dr = 4/3πr³
I don't think it means anything though. After all, you wouldn't say that the circumference of a sphere was 8π.
Why did the vector cross the road?
It wanted to be normal.
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That works, yes, but if r is the principle variable, then 2pi r is a line and pi r^2 is a parabola, so you aren't dealing with a circle, are you?
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Integrating a line equation gives the area below the curve (or line). The equation for the first quadrant is:
y = √r²-x²
Integrating this equation from zero to r gives:
x/2 (√r²-x²) + r²/2 (arcsin x/r) = πr²/4
Since this is only the area of one quadrant, you must multiply this by 4 which gives πr²
I am at an age where I have forgotten more than I remember, but I still pretend to know it all.
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Integrating a line equation gives the area below the curve (or line). The equation for the first quadrant is:
y = √r²-x²Integrating this equation from zero to r gives:
x/2 (√r²-x²) + r²/2 (arcsin x/r) = πr²/4
Since this is only the area of one quadrant, you must multiply this by 4 which gives πr²
Hi guys
Sorry to resurrect this thread but I really need to be able to derive the formula for the area of a circle using integration and I can't find anything useful on the internet. Please could you explain how it works without missing stages out so it's easier to follow. How do you integrate the "r"? I can't remember!
Thank you so much.
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If you want to do it this way (which is rather silly) oh well...
x^2+y^2=r^2
Find the area of the upper half:
y=sqrt(r^2-x^2) <--- equation for the upper half
integrate(sqrt(r^2-x^2)dx,x=-r..r) <---- inegrate from x=-r to x=r
use x=r*cos(theta) substitution. Notice if we want to integrate over theta, theta has to change from PI to 0, so that x=r*cos(theta) changes from r*cos(PI)=-r to r*cos(0)=r
then dx =-r*sin(theta)*d(theta)
sqrt(r^2-x^2) = sqrt(r^2-r^2*(cos(theta))^2)=r*sqrt(1-(cos(theta))^2)=r*sin(theta)
(we can do this because theta changes from 0 to PI and sine is always positive there)
So we have the following:
integrate(sqrt(r^2-x^2)dx,x=-r..r) = integrate(-r^2*[sin(theta)]^2(dtheta),theta=PI..0)=
=-r^2*[-PI/2] = PI*r^2/2. The total area is area of the upper half times two, i.e.
2 * [PI*r^2/2] = PI*r^2
How to evaluate int((sin(x))^2,x=0..PI): integrate by parts
int((sin(x))^2,x=0..PI) = -sin(x)*cos(x)|0,PI + int(cos(x)*cos(x),x=0..PI)
so int((sin(x))^2 dx,x=0..PI) = int((cos(x))^2 dx,x=0..PI)
thus
int((sin(x))^2,x=0..PI) = 1/2*int((sin(x))^2+(cos(x))^2 dx,x=0..PI) = 1/2*int(1 dx,x=0..PI)=
= 1/2 * PI
Integration by parts follows from the fact that
[f(x)*u(x)]' = f'(x)*u(x)+u'(x)*f(x)
f(x)=int(f'(x)), so
int(f'(x)*u(x)) = f(x)*u(x) - u'(x)*f(x). In the example above, I used f(x)=sin(x) and u(x)=sin(x), so that int(u(x)) = -cos(x) and u'(x) = cos(x)
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