# Introduction
The Poisson's equation is a second-order partial differential equation that stats the negative Laplacian $-\Delta u$ of an unknown field $u=u(x)$ is equal to a given function $f=f(x)$ on a domain $\Omega \subset \mathbb{R}^d$, most probably defined by a set of boundary conditions for the solution $u$ on the boundary $\partial \Omega$ of $\Omega$:

$$-\Delta u =f \quad \text{in } \Omega\text{,}$$
$$u=u_0 \quad \text{on } \Gamma_D \subset \partial\Omega \text{,}$$

here the Dirichlet's boundary condition $u=u_0$ signifies a prescribed values for the unknown $u$ on the boundary.

The Poisson's equation is the simplest model for gravity, electromagnetism, heat transfer, among others.

The specific case of $f=0$ and a negative $k$ value, leaves to the Fourier's Law.

## Comparative analysis
Along this example, the fenics platfomr is used to compare results obtained by solving the heat equation (Laplace equation) in 2-D:

$$\frac{\partial^2 T}{\partial x^2}+ \frac{\partial^2 T}{\partial y^2}=0$$

the problem is defined by the next geometry considerations:

![](physicalproblem.png)

The resulting contour of temperature, solving using finite diferences, is shown next:

![](resulteq.png)

# Solving by Finite Element Method with Varational Problem formulation


```python
#1 Loading functions  and modules
from fenics import *
import matplotlib.pyplot as plt
```


```python
#2 Create mesh and define function space
mesh = RectangleMesh(Point(0,0),Point(20,20),10, 10,'left')
V = FunctionSpace(mesh, 'Lagrange', 1) #Lagrange are triangular elements
plot(mesh)
plt.show()
```


![png](output_6_0.png)



```python
#3 Defining boundary conditions (Dirichlet)
tol = 1E-14 # tolerance for coordinate comparisons
#at y=20
def Dirichlet_boundary1(x, on_boundary):
    return on_boundary and abs(x[1] - 20) < tol
#at y=0
def Dirichlet_boundary0(x, on_boundary):
    return on_boundary and abs(x[1] - 0) < tol
#at x=0
def Dirichlet_boundarx0(x, on_boundary):
    return on_boundary and abs(x[0] - 0) < tol
#at x=20
def Dirichlet_boundarx1(x, on_boundary):
    return on_boundary and abs(x[0] - 20) < tol

bc0 = DirichletBC(V, Constant(0), Dirichlet_boundary0)
bc1 = DirichletBC(V, Constant(100), Dirichlet_boundary1) #100C
bc2 = DirichletBC(V, Constant(0), Dirichlet_boundarx0)
bc3 = DirichletBC(V, Constant(0), Dirichlet_boundarx1)
bcs = [bc0,bc1, bc2,bc3]
```


```python
#4 Defining variational problem and its solution
k =1
u = TrialFunction(V)
v = TestFunction(V)
f = Constant(0)
a = dot(k*grad(u), grad(v))*dx
L = f*v*dx

# Compute solution
u = Function(V)
solve(a == L, u, bcs)

# Plot solution and mesh
plot(u)
plot(mesh)

# Save solution to file in VTK format
vtkfile = File('solution.pvd')
vtkfile << u
```


![png](output_8_0.png)


# Results after editing color-map on paraview
![](paraview-results.png)