7.1.17 int e^{-\dfrac{x^2}{2}} dx from 0 to infty

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Discussion Overview

The discussion revolves around evaluating the integral $\displaystyle\int_0^\infty e^{-\dfrac{x^2}{2}} dx$. Participants explore various methods for solving this integral, including integration by parts, comparisons with known integrals, and a clever use of polar coordinates.

Discussion Character

  • Exploratory
  • Mathematical reasoning

Main Points Raised

  • One participant suggests using integration by parts (IBP) and questions whether to use $e^u$ with $u=-\dfrac{x^2}{2}$ or $u=\dfrac{x}{\sqrt{2}}$.
  • Another participant notes the known result $\displaystyle \int_{-\infty}^{\infty}{\mathrm{e}^{-x^2}\,\mathrm{d}x} = \sqrt{\pi}$ and derives that $\displaystyle \int_0^{\infty}{\mathrm{e}^{-x^2}\,\mathrm{d}x} = \frac{\sqrt{\pi}}{2}$, leading to the conclusion that $\displaystyle \int_0^{\infty}{ \mathrm{e}^{-\frac{x^2}{2}}\,\mathrm{d}x } = \frac{\sqrt{2\,\pi}}{2}$ due to dilation.
  • A participant expresses gratitude for the information shared, indicating it aids in solving the problem.
  • Another participant presents a method involving squaring the integral and converting to polar coordinates, ultimately leading to the result of $2\pi$ for the squared integral.

Areas of Agreement / Disagreement

Participants present different methods for evaluating the integral, with no consensus on a single approach. Multiple competing views remain regarding the best method to solve the integral.

Contextual Notes

The discussion includes various assumptions about the properties of integrals and transformations, but these are not resolved or universally accepted among participants.

karush
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Evaluate $\displaystyle\int_0^\infty e^{-\dfrac{x^2}{2}} dx$

ok first reponse is use IBP but can we use $e^u$ where $u=-\dfrac{x^2}{2}$ ot $u=\dfrac{x}{\sqrt{2}}$
 
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It's well known that $\displaystyle \begin{align*} \int_{-\infty}^{\infty}{\mathrm{e}^{-x^2}\,\mathrm{d}x} = \sqrt{\pi} \end{align*}$, and due to the evenness of this function, that means $\displaystyle \begin{align*} \int_0^{\infty}{\mathrm{e}^{-x^2}\,\mathrm{d}x} = \frac{\sqrt{\pi}}{2} \end{align*}$.

If we compare the functions $\displaystyle \begin{align*} f\left( x \right) = \mathrm{e}^{-x^2} \end{align*}$ and $\displaystyle \begin{align*} g\left( x \right) = \mathrm{e}^{-\left( \frac{x}{\sqrt{2}} \right) ^2 } \end{align*}$, we can see that $\displaystyle \begin{align*} g\left( x \right) \end{align*}$ is the image of $\displaystyle \begin{align*} f\left( x \right) \end{align*}$ after a dilation by factor $\displaystyle \begin{align*} \sqrt{2} \end{align*}$ from the $\displaystyle \begin{align*} y \end{align*}$ axis. Therefore, their integrals are also dilated by factor $\displaystyle \begin{align*} \sqrt{2} \end{align*}$.

Therefore $\displaystyle \begin{align*} \int_0^{\infty}{ \mathrm{e}^{-\frac{x^2}{2}}\,\mathrm{d}x } = \sqrt{2}\cdot \frac{\sqrt{\pi}}{2} = \frac{\sqrt{2\,\pi}}{2}\end{align*}$.
 
actually i didn't know that...
but sure helps in solving the problem
much Mahalo
 
Here is the rather clever way that integral can be done.
Let [math]I= \int_0^\infty e^{-\frac{x^2}{2}} dx[/math].
Then [math]I= \int_0^\infty e^{-\frac{y^2}{2}} dy[/math] since that is just changing the name of the "dummy variable".

So [math]I^2= \left( \int_0^\infty e^{-\frac{x^2}{2}} dx\right)\left(\int_0^\infty e^{-\frac{y^2}{2}} dy\right)[/math]
[math]I^2= \int_0^\infty\int_0^\infty e^{-6\frac{x^2+ y^2}{2}} dxdy[/math].

To integrate that, change to polar coordinates! Since x goes from 0 to infinity and y goes from 0 to infinity, covering the first quadrant, in polar coordinates r goes from 0 to infinity and [math]\theta[/math] goes from 0 to [math]\frac{\pi}{2}[/math]. [math]x^2+ y^2= r^2[/math] and [math]dxdy= rdrd\theta[/math].

The integral becomes [math]\int_0^{2\pi}\int_0^\infty e^{-\frac{r^2}{2}}rdrd\theta[/math]
[math]= 2\pi\int_0^\infty e^{-\frac{r^2}{2}}rdr[/math]

Now let [math]u= \frac{r^2}{2}[/math] so that [math]du= r dr[/math] so the integral becomes
[math]2\pi\int_0^\infty e^{-u}du= 2\pi\left[-e^{-u}\right]_0^\infty= 2\pi\left[-(0- 1)\right]= 2\pi[/math].
 

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