The Dirichlet difference problen:1 for Poisson's equation 243
domain. We follow the second way of approximating the Laplace operator
on an irregular pattern (see Fig. 8). The expression
* _ 2_ [ v( +^1 ") - v _ v - v( -l.,) l
(16) Aa v - h (\' h (\' +. h (\' - ,
reveals A~ instead of formula (14) as
A* a v = !i(\' h Vx;,,;:.,.
(\'
We claim that in this case the operator A~ generates the local approxima-
tion of zero order
1/Ja = A~u -Aau = 0(1).
Indeed, taking into account (15) we arrive at the chain of the relations
We clarify the situation, in which approximation (16) is quite applicable,
on the basis of one possible example.
Example For the boundary-value problem
u" = - f(x), O<x<l, u(O)=O, u(l)=O,
we form the grid
which is everywhere equidistant, but near the boundary h 1 < h, h 2 < h,
h 1 + h 2 + (N - l)h = 1. At the regular nodes xi, 1 < i < N, we find that
ui+1 - 2ui + ui-1
h2