What is the solution to the Gaussian integral?

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Homework Help Overview

The problem involves evaluating the integral ##\displaystyle\int_{-\infty}^{\infty} 3e^{-8x^2}dx##, which is related to the Gaussian integral. Participants reference known results about Gaussian integrals and discuss various approaches to solve the problem.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss using substitution and changing to polar coordinates as potential methods. Some express uncertainty about how to properly show their reasoning or derive the results. Others question the validity of using known formulas versus deriving results from first principles.

Discussion Status

The discussion includes multiple interpretations and approaches, with some participants sharing their reasoning and results. There is no explicit consensus, but several productive lines of inquiry are being explored, including the use of double integrals and polar coordinates.

Contextual Notes

Participants mention the importance of understanding the derivation of the Gaussian integral and express a desire to work through the problem without relying solely on known results. There is also a recognition of the constraints imposed by homework rules and the need to show work clearly.

jonroberts74
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Homework Statement



I am asked to evaluate ##\displaystyle\int_{-\infty}^{\infty} 3e^{-8x^2}dx##

Homework Equations



I know

##\displaystyle\int_{-\infty}^{\infty} e^{-x^2}dx = \sqrt{\pi}##


The Attempt at a Solution


based on an example in the book it seems a change of variables is what I need to do.

I'm just not sure how
 
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I figured it out

##3\sqrt{\frac{\pi}{8}}##

still a bit puzzled on how I show that though
 
Have you tried substitution?
 
You can try setting it up as a double integral and doing it in polar coordinates.
 
jonroberts74 said:
I figured it out

##3\sqrt{\frac{\pi}{8}}##

still a bit puzzled on how I show that though

Now I'm puzzled. You figured it out but now you don't know how you did it?
 
LCKurtz said:
Now I'm puzzled. You figured it out but now you don't know how you did it?

I used what I knew of the gaussian integral

and when it is of the form ##\displaystyle\int_{-\infty}^{\infty} e^{-ax^2}dx##

the answer is ##\sqrt{\frac{\pi}{a}}## and the 3 is just a constant so that factored out of the integral

so ##3\sqrt{\frac{\pi}{8}}##

I'll try it with polar coordinates though, this way was a bit like "cheating"
 
Guess I am going to give it a go.You can set it up as

\displaystyle\int^{\infty}_{-\infty}\int^{\infty}_{-\infty}e^{-8x^{2}-8y^{2}}dxdy

Now this can be rewritten as

\displaystyle\int^{\infty}_{-\infty}e^{-8y^{2}}\int^{\infty}_{-\infty}e^{-8x^{2}}dxdy

If we label the original integral A solving this double integral will give us A^{2}, so if we manage to solve it we can just take the square root and get our answer.

Let's use polar coordinates then our integral becomes

\displaystyle\int^{\infty}_{0}\int^{2\pi}_{0}re^{-8r^{2}}d\theta dr =

= 2 \pi \displaystyle\int^{\infty}_{0}re^{-8r^{2}}dr =

= \left[ 2 \pi \frac{(-e^{-8r^{2}})}{16} \right]_{0}^{\infty} = \frac{\pi}{8}

So A = \sqrt{\frac{\pi}{8}}
 
Last edited:
No, using the fact that \int 3 f(x)dx= 3\int f(x)dx is NOT cheating!

If you are concerned about how they got that \int_{-\infty}^\infty e^{-ax^2} dx= \sqrt{\pi/a}-

Do you know how to show that \int_{-\infty}^\infty e^{-x^2}dx= \sqrt{\pi}? If not, "set it up as a double integral and change to polar coordinates" as exo suggested. Once you know that, because you have e^{-ax^2} and want e^{-u^2} use the substitution -u^2= ax^2 or u= \sqrt{a} x.
 
HallsofIvy said:
No, using the fact that \int 3 f(x)dx= 3\int f(x)dx is NOT cheating!

If you are concerned about how they got that \int_{-\infty}^\infty e^{-ax^2} dx= \sqrt{\pi/a}-

Do you know how to show that \int_{-\infty}^\infty e^{-x^2}dx= \sqrt{\pi}? If not, "set it up as a double integral and change to polar coordinates" as exo suggested. Once you know that, because you have e^{-ax^2} and want e^{-u^2} use the substitution -u^2= ax^2 or u= \sqrt{a} x.


I didn't mean cheating was about pulling the constant outside the integral. I meant I'd rather work the problem out properly than use a known formula to get skip to the end. And of course that isn't cheating either, more so cheating myself of the fun of solving a neat integral.

I did it using polar coordinates, I got to the same answer.
 
  • #10
jonroberts74 said:
...

I did it using polar coordinates, I got to the same answer.
Let's see the details of that!

I'm intrigued .
 
  • #11
SammyS said:
Let's see the details of that!

I'm intrigued .


I'll let G = ##\int_{-\infty}^{\infty} 3e^{-8x^2}dx##

and ##G^2 =\int_{-\infty}^{\infty} \int_{-\infty}^{\infty}9e^{-8(x^2+y^2)}dxdy##

Changing to polar

##\int_{0}^{2\pi} \int_{0}^{\infty}9e^{-8r^2}rdrd\theta##

the outside integral doesn't rely and is not affect by the one on the inside

##\int_{0}^{2\pi} d\theta \int_{0}^{\infty}9e^{-8r^2}rdr##

I'm going to introduce the limit now, previously left out for expedience

##2\pi\Bigg[\lim_{a \to \infty}\int_{0}^{\infty}9e^{-8r^2}rdr\Bigg]##

##9*2\pi\Bigg[\lim_{a \to \infty}\int_{0}^{\infty}e^{-8r^2}rdr\Bigg]##

##u=8r^2; du=16rdr \rightarrow \frac{du}{16r}=dr##

##9*2\pi\Bigg[\lim_{a \to \infty}\int_{0}^{\infty}e^{-u^2}r\frac{du}{16r}\Bigg]##

##9*2\pi\Bigg[\lim_{a \to \infty}\frac{1}{16}\int_{0}^{\infty}e^{-u^2}du\Bigg]##

##9*2\pi \Bigg[\lim_{a \to \infty}\frac{1}{16}(-e^{-8x^2})\Bigg|_{0}^{a}\Bigg]##

##9\Bigg[\lim_{a \to \infty}\frac{\pi}{8}(-e^{-8a^2}+e^{0})\Bigg]##

##9\cdot\frac{\pi}{8} = G^2##

##3\sqrt{\frac{\pi}{8}}=G##
 
  • #12
jonroberts74 said:
I'll let G = ##\int_{-\infty}^{\infty} 3e^{-8x^2}dx##

and ##G^2 =\int_{-\infty}^{\infty} \int_{-\infty}^{\infty}9e^{-8(x^2+y^2)}dxdy##

Changing to polar

##\int_{0}^{2\pi} \int_{0}^{\infty}9e^{-8r^2}rdrd\theta##

the outside integral doesn't rely and is not affect by the one on the inside

##\int_{0}^{2\pi} d\theta \int_{0}^{\infty}9e^{-8r^2}rdr##

I'm going to introduce the limit now, previously left out for expedience

##2\pi\Bigg[\lim_{a \to \infty}\int_{0}^{\infty}9e^{-8r^2}rdr\Bigg]##

##9*2\pi\Bigg[\lim_{a \to \infty}\int_{0}^{\infty}e^{-8r^2}rdr\Bigg]##

##u=8r^2; du=16rdr \rightarrow \frac{du}{16r}=dr##

##9*2\pi\Bigg[\lim_{a \to \infty}\int_{0}^{\infty}e^{-u^2}r\frac{du}{16r}\Bigg]##
You mean "\lim_{a\to\infty}\int_0^a".

##9*2\pi\Bigg[\lim_{a \to \infty}\frac{1}{16}\int_{0}^{\infty}e^{-u^2}du\Bigg]##

##9*2\pi \Bigg[\lim_{a \to \infty}\frac{1}{16}(-e^{-8x^2})\Bigg|_{0}^{a}\Bigg]##

##9\Bigg[\lim_{a \to \infty}\frac{\pi}{8}(-e^{-8a^2}+e^{0})\Bigg]##

##9\cdot\frac{\pi}{8} = G^2##

##3\sqrt{\frac{\pi}{8}}=G##
 
  • #13
Oops, yeah thanks. It was the end of the night. Its worked out properly on paper.
 
Last edited:

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