|
|
Subject:
Integral from 1958
Category: Science > Math Asked by: missionpeak-ga List Price: $10.00 |
Posted:
17 Aug 2004 21:32 PDT
Expires: 20 Aug 2004 21:21 PDT Question ID: 389311 |
I've been studying probability on my own using an old textbook (~1958). One of the problems reduces to showing that the result of an integral equals the gaussian density function. I can use various computational methods to prove that the integral does in fact equal the guassian density function, but I have no idea how to evaluate the integral using techniques available in 1958. Out of curiosity, I'd be very happy if someone could show me how. Here is the integral: Int[abs(k) to inf] ((x*E^(-(1/2)*x^2)) / (Pi*Sqrt[x^2 - k^2])) dx This does in fact equal the gaussian density function of k: E^(-(1/2)*k^2) / Sqrt[2*Pi] Can you prove this using only techniques available to a college student in 1958? Thanks! | |
| |
|
|
There is no answer at this time. |
|
Subject:
Re: Integral from 1958
From: kprema-ga on 18 Aug 2004 05:39 PDT |
Hi: Let us first look at the case when k >= 0. The integral then is (1) I = \int_{x=k}^{inf} x*exp(-x^2/2)/(pi*sqrt(x^2-k^2)) dx. Use the substitution u^2 = x^2 - k^2 --> u du = x dx. Then we have (2) I = exp(-k^2/2)/pi * \int_{u=0}^{inf} exp(-u^2/2) du. But, it is well established that (check a handbook on integrals) (3) \int_{u=0}^{inf} exp(-a^2*u^2) du = sqrt(pi)/(2*a), for a > 0. When a = 1/sqrt(2), this reduces to (4) \int_{u=0}^{inf} exp(-u^2/2) du = sqrt(pi/2). This is exactly the integral that appears in (2). Hence, we have (5) I = exp(-k^2/2)/sqrt(2*pi), which is what you wanted I think. Now, let us look at the case when k < 0. The integral then reduces to an expression that is identical to (1) except that the integration limits are from -k to inf (instead of k to inf). But, when the substitution u^2 = x^2 - k^2 is made, one is left with (2). Hence, the result is the same. I hope this helps. kprema |
Subject:
Re: Integral from 1958
From: mathtalk-ga on 18 Aug 2004 05:58 PDT |
Hi, kprema: The original integral uses |k| as the lower limit of integration (and only k^2 appears within the integral). So you can consider only k >= 0 and know that the result depends only on |k|, i.e. an even function of k. Your u-substitution (1) is a bit different than the one I had in mind (see above), and I like it. There is a way to evaluate (4) without appealing to a handbook, but the "trick" requires stepping up to two dimensions. regards, mathtalk-ga |
Subject:
Re: Integral from 1958
From: kprema-ga on 18 Aug 2004 06:16 PDT |
Hi mathtalk-ga: You are right, and may I also thank you for the inspiring discussions. I was actually about to show how to do the integral when I realized that you had posted a comment. In any case, let me include the derivation (at laest for the sake of completeness): First, let (1) I = \int_{x=0}^{inf} exp(-x^2) dx. Then (2) I^2 = \int_{y=0}^{inf} \inf_{x=0}^{inf} exp(-(x^2+y^2)) dx dy. Use the following "polar" coordinate substitution: (3) x^2+y^2 = r^2, x = r*cos(theta), y=r*sin(theta). This yields (4) I^2 = \int_{theta=0}^{pi/2} \int_{r=0}^{inf} exp(-r^2)*r dr dtheta, where the "extra" r term on the right-hand-side is generated from the corresponding Jacobian, i.e., (5) det([dx/dr dx/dtheta; dy/dr dy/dtheta]) = r. So, let us get back to (4). Integrate out theta to get (6) I^2 = (pi/2) \int_{r=0}^{inf} r*exp(-r^2) dr. Substitute r^2 = x --> 2*r dr = dx: (7) I^2 = pi/4 --> I = sqrt(pi)/2. Remember that, what we wanted was an expression for (8) J = int_{x=0}^{inf} exp(-a^2*x^2) dx. Well, with (7) in hand, this is quite easy when one uses the substitution (9) a*x = y with a > 0. Note: It is essential that a > 0 to keep the integration sensible. kprema |
If you feel that you have found inappropriate content, please let us know by emailing us at answers-support@google.com with the question ID listed above. Thank you. |
Search Google Answers for |
Google Home - Answers FAQ - Terms of Service - Privacy Policy |