a>0. integrate from 0 to infinity of e^(-ax^2)
Uh, I think it's \(\large \sqrt{\frac{\pi}{4a}}\).
i cannot understand it, how we know that
I thought you wouldn't. Do you know \(\large \int_0^{\infty}e^{-x^2}\mathrm{d}x\) ?
no.
Ok, so I will show you how to find that, and then you can find your answer easily.
should have put 2 outside the root
So consider the following integral:\[\int_0^{\infty}\int_0^{\infty} e^{-x^2-y^2}dy~dx=\int_0^{\infty}\int_0^{\infty} e^{-x^2}e^{-y^2}dy~dx=\int_0^{\infty}e^{-x^2}\int_0^{\infty} e^{-y^2}dy~dx\]\[=\left (\int_0^{\infty}e^{-x^2}dx\right ) \left (\int_0^{\infty} e^{-y^2}dy\right ) =\left (\int_0^{\infty}e^{-x^2}dx\right )^2\]
in second last step, do we consider y = x?
@eamier Well, x and y are both "dummy variables". The value of a definite integral does NOT depend on what variable we are using. It is simply a number. It depends on the function and the region of integration. So, if we find the volume under the surface e^(-x^2-y^2) in the first quadrant, we have found the square of our desired integral. (I hope you understand volume integrals. If not, look in your textbook or whatevs.) Now \(-x^2-y^2=-\left ( x^2+y^2\right ) =-\left ( \sqrt{x^2+y^2}\right ) ^2=-r^2\), where r is the distance from the origin, used in polar coordinates.
So the surface depends only on r. Not on Θ. You should realize that this means the surface is a surface of revolution. You probably studied such surfaces in Calc 1. What we have is a function z=f(r) rotated around the z axis.
But we only need one fourth of the entire volume.
Do you think you can get it from there?
this really has nothing to do with when you integrate e, divide by the derivative of it power..i really cant imagine it. but how we get the pi
Or take: \[\int_0^{\pi/2}\int_0^{\infty}e^{-r^2}r~dr~d\theta\]This is a simple polar integral which represents the volume under \(e^{-x^2-y^2}\) in the first quadrant. I know it may seem strange, but the math is flawless. You get the pi because multiplying \(e^{-x^2}\) with \(e^{-y^2}\) just so happens to give you \(e^{-r^2}\), and anything to do with polar coordinates usually has to do with pi. You will find that the above integral is equal to \(\frac{\pi}{4}\). Once you know that integral, you can use simple substitutions to find your original integral. Do you need help with the above integral?
i tried but cant do even this part\[\int\limits_{0}^{\infty}e ^{-r ^{2}}rdr\].
let r^2 = u 2rdr = du
done. tq
Join our real-time social learning platform and learn together with your friends!