The finite difference method is a very useful tool for discretizing and solving numerically a differential equation. It is effectively a classical method of approximation based on Taylor series expansions that has help during the last years theoretical results to gain in accuracy, stability and convergence.

In fact, this method is very useful for solving for example Poisson equation. This elliptic equation appears very often in mathematics, physics, chemistry, biology and engineering. In one dimension, the resolution leads to a tridiagonal matrix in the case of centered difference approximation. This matrix, which is diagonally dominant, can be inverted with methods such as Gauss elimination, Thomas Algorithm Method [1] . These technics are powerful and very efficient.

We proposed here, a new and direct method of inversion of this tridiagonal matrix independently of the right- hand side. For Dirichlet-Dirichlet boundary problems, this innovative method is faster than the Thomas Algorithm. It gives better accuracy and is far more economical in terms of memory occupation.

First, the finite difference method is presented for the 1D Poisson equation. Secondly, the properties of the matrix associated with the Laplacian and its inverse are discussed. Then, the inverse matrix is determined and its properties are analyzed. Thus, verification is done considering an interesting potential problem, and the sensibility of the method is quantified.

We consider a function which satisfies the Poisson equation, in the interval, where is a specified function. fulfills the Dirichlet-Dirichlet boundary conditions and. We consider an one-dimensional mesh with discrete points. Each point is de-

fined by, where being the step size. We define, ,.

We have chosen the centered difference approximation, in this work, for the fact that it gives a tridiagonal, diagonally dominant, and symmetric matrix. Considering all the above mentioned criteria, one can rewrite the 1D Poisson equation in a set of algebraic equations:

One gets a linear system of equations, which can be written in a matrix form [2]

Thus, solving the 1D Poisson equation means to invert the negative definite, and regular -matrix. Its inverse, that we noted, is also symmetric. Both matrices have the following properties:

and

where is the Kronecker’s delta.

From (4), we derive successively the following interesting relations:

with (5), one sees that the matrix is entirely determined if the term is known. This term can be determined by observing the behavior of for different values: It holds

From (5) and (6), we get

Now, the matrix is completely and exactly determined. with

The solution of the 1D Poisson equation is obtained with a simple, extremely fast matrix multiplication:. Thus, the numerical resolution of the 1D Poisson equation which is an interesting topic in physics and engineering is made easy and very accurate.

A first analysis of the matrix let us believe that, this new method possesses an algorithm complexity of, which is situated between the Gauss eliminations and the one of Thomas’s [1] .

A deeper analysis of the matrix shows that the complexity brought by the Thomas method is largely improved in this study. In addition, one can see a close link between its row vectors and column vectors.

The matrix is also persymmetric:

All the information about it, can be found in the upper triangle (in gray color, see Figure 1).

Further, we can even find very interesting relations in this matrix which can help refining the final solution.

That is what we effectively did, and one can see a direct solution for at the point, which can be expressed by

Also a direct solution for at the point is:

Generally, a very important recurrence relation can be obtained, which gives all solutions:

which is equivalent to:

This very innovative Equation (12) gives directly and accurately all the solution that we are looking for. It proves that our method is direct, faster than the one of Thomas’s in this context and gives as well better accuracy. Furthermore, it is far more economical in terms of memory occupation. This is due to the fact that the matrix does not necessitate to be generated. A programmer does not need to declare nor to define the matrix in his code.

In conclusion to this, we can say that the matrix is the key of this efficient new method. This matrix, which is the inverse of matrix, is determined explicitly, directly, and independently of the right-hand side of the Poisson equation.

N.B.: One can prove using mathematical induction that. It holds for the cofactor of:. We call the matrix Bira’s Matrix.

We consider a scalar potential, defined in [0, 1], which satisfies

. fulfills the following boundary conditions:

. The exact solution is

With the finite difference method, we take, , , , and. The solution is

We define the variable, which is the relative error at point for. represents.

Generally, we have

We can also define the average value of the relative error for a given:. For, it is:.

We obtain the following results, presented in Table 1.

The table shows that the solution is very accurate. Notwithstanding that we have been interested in determining the sensibility of the proposed method. Effectively, we have plotted for different values.

We obtain a hyperbola, which can be predicted as proportional to.

This curve is fitted with a function which can be defined as

where. We obtain two curves represented in Figure 2.

We realize that the average relative error behaves like a truncation error that we express in the fol-

lowing manner. is the fourth order derivative of the function in a point (here) which belongs to the interval.

For our given function and also the results from the fitting, we have the following relations [3] :

This proves that the method is very accurate, naturally stable, robust, quick and precise.

This paper has provided a new improved method for solving the 1D Poisson equation with the finite difference

method. Accurate results have been obtained with a sensibility found to be as the function of. In fact, the inverse of the tridiagonal matrix, which is associated with this differential equation, is determined directly, exactly, and independently to the right-hand side. Thus, a new formulation of the solution is given with an algorithmic complexity of O(N). With this innovative method, the 1D Poisson equation, with Dirichlet-Dirichlet boundary condition is solved, with only one programming loop. This new approach provides also gain in accuracy and economy in memory allocation.

A future work can consider Neumann or mixed boundary conditions.

I would like to thank my colleagues Dr. Cheikh Mbow and Dr. Kharouna Talla for benefit discussions and remarks that contribute to improving the quality of this paper.