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.
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!
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.
I think you call this PDE, the heat equation btw
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!
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.
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).
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!
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!
Yea, i'll probably end out brute focing my way through this, i just thought it'd be cool to learn a new approach :)
thank you very much for your help :)
You're welcome!
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