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Mathematics 21 Online
OpenStudy (anonymous):

Is it possible to show, that this http://prntscr.com/2zbunw is a solution to the PDE http://prntscr.com/2zbuze With fourier transform/Laplace transform. If it's possible how should i start out.

OpenStudy (accessdenied):

I have a few observations while I look into this further: (1) The original PDE does not specify any initial/boundary conditions? If I recall, Laplace transforms make use of that and I imagine the Fourier transform does too. (2) The given solution seems like a particular solution (it does not have any variables except those from the initial equation. Anyone more familiar with this can comment better than I can, though!

OpenStudy (anonymous):

it's a particular solution for the probability density function P(x,t), with boundry conditions x=0 for small t. If im right, i can't find the exact boundry conditions.

OpenStudy (anonymous):

I think you call this PDE, the heat equation btw

OpenStudy (accessdenied):

Yeah, 1D Heat Equation compares correctly to me. Wirh Laplace Transform, I can see this: \( \displaystyle \frac{\partial P}{\partial t} = D \frac{\partial ^2 P}{\partial x^2 } \) \( \displaystyle \frac{\partial P}{\partial t} e^{-st} \; \text{d}t = D \frac{\partial ^2 P}{\partial x^2} e^{-st} \; \text{d} t \) \( \displaystyle \mathcal{L} \left[ \frac{\partial P}{\partial t} \right] = s \mathcal{L} \left[ P \right] - P(x, 0) \) and then \( \displaystyle \mathcal{L} \left[ D \frac{\partial^2 P}{\partial x^2} \right] = D \frac{\text{d}^2}{\text{d}x^2} \left( \mathcal{L} \left[ P \right] \right) \) the key note to worry of is the appearance of P(x,0). We at least know t goes from 0 to infinity so right-hand limit as t goes to 0. That all seems reasonable to me. (Am reading through this: http://science.uwaterloo.ca/~suwingspany/earth661/pdfs/6-1_ES661_W2008_06_Chapter_06.pdf) Again, will say I have not done much with Laplace transform for partial derivatives / PDE so definitely go over anything I write carefully!

OpenStudy (accessdenied):

http://science.uwaterloo.ca/~suwingspany/earth661/pdfs/6-1_ES661_W2008_06_Chapter_06.pdf original link has a ) at the end so it breaks.

OpenStudy (anonymous):

Thank you, i just have to understand this, i havn't had any training in fourier transform or anything like that yet. I just read somewhere that it'd be easier to prove that P is a solution to the PDE with fourier transform, instead of doing the plug-n-chug method (inserting the solution into the PDE).

OpenStudy (accessdenied):

Ah, alright. No problem. Have you had work with Laplace transform in the past, though? Fourier transform is for the most part like a special case of Laplace transform (that is, s = a + wi but a=0 for Fourier). I just have not used Fourier transforms as often as Laplace when I was going over it on my own time!

OpenStudy (accessdenied):

Got it. Anyways, best of luck with your studies! :) I personally prefer plug n chug on anything because I just brute force things, but I do know Laplace/Fourier are powerful transforms in ODE/PDE once you know their properties!

OpenStudy (anonymous):

Yea, i'll probably end out brute focing my way through this, i just thought it'd be cool to learn a new approach :)

OpenStudy (anonymous):

thank you very much for your help :)

OpenStudy (accessdenied):

You're welcome!

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