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The resolution is simple. Simply specify the value at one point, say, (ax, ay) to be any value that you like, such as zero.
Another artifice is to use v = u/x ( or, if better suited, u/y) as the dependent variable.
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That is the Poisson equation, not the Helmholtz equation -- the latter has the additional term q . u in it, where q is a constant. Please clarify which equation you want to solve.
And, when you wrote in your first post that
> The problem is that my function is not defined on boundaries
did you refer to u or to F as "my function" ?
In the problem that you want to solve, is F known as an analytical expression? If not, how is it known?
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Gents,
It's seems we have some misunderstanding. For differential problem one doesnt know values of rhs on boundary of domain. But for algebraic problem that comes from differential one need to set value on boundary (for example continue rhs from domain to its boundary).
With best regards,
Alexander Kalinkin
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Ilia,
MKL uses a standard 5-point approximation of 2D Helmholtz problem. But Poisson library from MKL requires values of rhs on Neumann boundary to find values of solution on this boundary. So, if you want to use Helmholtz functionality you need to implement next trick:
If want to solve Helmholtz equation in domain (a_x, b_x)*(a_y, b_y) with nx and ny mesh intervals correspondently then call Poisson library with parameters as follows:
ax_new = a_x+(bx-ax)/nx;
bx_new = b_x-(bx-ax)/nx;
ay_new = a_y+(by-ay)/ny;
by_new = b_y-(by-ay)/ny;
nx_new = nx-2;
ny_new = ny-2;
d_init_Helmholtz_2D(&ax_new, &bx_new, &ay_new, &by_new, &nx_new, &ny_new, BCtype, &q, ipar, dpar, &stat);
d_commit_Helmholtz_2D(f, bd_ax, bd_bx, bd_ay, bd_by, &xhandle, ipar, dpar, &stat);
ets
With best regards,
Alexander Kalinkin
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