n this section we present a general way to construct a finite difference
approximation for a solution of the heat equation via a procedure with linear
dependency of the amount of computation on the size of the lattice.
We are considering the following boundary problem for the heat
equation:  
We introduce the uniform
lattices
the lattice function
and notation
.
The introduced above notations
and
refer to the
-variable.
Consider the
scheme | | (Alternating directions1) |
 | | (Alternating directions2) |
in all internal points of the lattice
.
The
refers to the operator
acting in the
index. The initial conditions
are
and the boundary conditions
are | | (Alternating boundary1) |
 | | (Alternating boundary2) |
The key observation about the scheme
( Alternating
directions1)-( Alternating boundary1)
is that the ( Alternating directions1)
is a one dimensional implicit scheme in the
-direction
while the ( Alternating directions2) is
the implicit scheme in the
-direction.
Hence, starting from
we use ( Alternating directions1) to
find the
through the factorization procedure of the previous section. Afterwards, we
similarly use ( Alternating
directions2) to find
.
To understand the boundary condition
( Alternating boundary1) subtract
( Alternating directions1) from
( Alternating directions2) and obtain
 | | (Alternating boundary) |
|