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Go back to [[Medusa#Examples|Examples]]. | Go back to [[Medusa#Examples|Examples]]. | ||
Our library natively supports complex numbers. | Our library natively supports complex numbers. To demonstrate this a simple example of Poisson's equation is presented below. For more complicated complex-valued problems see [[Electromagnetic scattering]] and [[Schrödinger equation]]. | ||
== 2D Complex Poisson's equation == | |||
We are solving 2D complex Poisson equation, on a unit square with Dirichlet boundary conditions | |||
\[ | |||
\begin{align*} | |||
i \Delta u &= f &&\text{in } \Omega, \\ | |||
u &= 0 &&\text{on } \partial \Omega, | |||
\end{align*} | |||
\] | |||
where $u(x,y)$ is the solution to the problem and $\Omega = [0, 1] \times [0, 1]$ denotes the square domain. We will consider $f(x,y) = 2\pi^2\sin(\pi x)\sin(\pi y)$, as it makes for | |||
a simple solution $u(x,y) = i\sin(\pi x)\sin(\pi y)$. | |||
We write the equations for our problem by directly translating the mathematical formulation above into code. | |||
<syntaxhighlight lang="cpp"> | |||
for (int i : domain.interior()) { | |||
double x = domain.pos(i, 0); | |||
double y = domain.pos(i, 1); | |||
1.0_i * op.lap(i) = -2*PI*PI*sin(PI * x)*sin(PI * y); | |||
} | |||
for (int i : domain.boundary()) { | |||
op.value(i) = 0.0; | |||
} | |||
</syntaxhighlight> | |||
The solution $u(x,y)$ is plotted below. In our case solution consist only of the imaginary part, the real part is equal to zero. | |||
[[File:complex_poisson_2D_real.png|500px]] | |||
[[File:complex_poisson_2D_imag.png|500px]] | |||
Go back to [[Medusa#Examples|Examples]]. | Go back to [[Medusa#Examples|Examples]]. | ||
Revision as of 14:04, 19 July 2019
Go back to Examples.
Our library natively supports complex numbers. To demonstrate this a simple example of Poisson's equation is presented below. For more complicated complex-valued problems see Electromagnetic scattering and Schrödinger equation.
2D Complex Poisson's equation
We are solving 2D complex Poisson equation, on a unit square with Dirichlet boundary conditions
\[ \begin{align*}
i \Delta u &= f &&\text{in } \Omega, \\
u &= 0 &&\text{on } \partial \Omega,
\end{align*} \] where $u(x,y)$ is the solution to the problem and $\Omega = [0, 1] \times [0, 1]$ denotes the square domain. We will consider $f(x,y) = 2\pi^2\sin(\pi x)\sin(\pi y)$, as it makes for a simple solution $u(x,y) = i\sin(\pi x)\sin(\pi y)$.
We write the equations for our problem by directly translating the mathematical formulation above into code.
for (int i : domain.interior()) {
double x = domain.pos(i, 0);
double y = domain.pos(i, 1);
1.0_i * op.lap(i) = -2*PI*PI*sin(PI * x)*sin(PI * y);
}
for (int i : domain.boundary()) {
op.value(i) = 0.0;
}
The solution $u(x,y)$ is plotted below. In our case solution consist only of the imaginary part, the real part is equal to zero.
Go back to Examples.