Replies: 1 comment
-
I'm afraid that such a special case will be not straight-forward to implement in |
Beta Was this translation helpful? Give feedback.
0 replies
Sign up for free
to join this conversation on GitHub.
Already have an account?
Sign in to comment
Uh oh!
There was an error while loading. Please reload this page.
Uh oh!
There was an error while loading. Please reload this page.
-
Hi, thank you so much for such an amazing package!
I apologize if the question is very basic, I'm still new with the use of this package. I'm trying to solve a Fokker-Planck equation in 2+1 D of the form$\partial_t P(x,y,t) = \frac{D}{2} \partial_x^2 P - f1(x,y,t) \partial_x P + f2(x,y) \partial_y P + f3(x) P$ . The range of x goes from -$\infty$ to xT, and y goes form -$\infty$ to $\infty$
There is an absorbing boundary for x = xT so P(xT,y,t) = 0, but I want to reinsert the flux through this boundary in x=xR. Thus, there will be a discontinuity in the derivative at x=xR:$\partial_x P(x=xR^+,y,t) - \partial_x P(x=xR^-,y,t) = \partial_x P(x=xT,y,t)$ , and the function P will be continuous at x=xR.
So I'm thinking in separating the plane in two regions, one for x=xR. But I don't know how to write the boundary conditions at the interface x=xR (the two conditions are continuity in x=xR and a jump in the first derivative)
I'd really appreciate if someone can help me with this
Beta Was this translation helpful? Give feedback.
All reactions