An inverse problem concerning the two-dimensional diffusion equation with s
ource control parameter is considered. Four finite-difference schemes are p
resented for identifying the control parameter which produces, at any given
time, a desired energy distribution in a portion of the spatial domain. Th
e fully explicit schemes developed for this purpose, are based on the (1, 5
) forward time centred space (FTCS) explicit formula, and the (1, 9) FTCS s
cheme, are economical to use, are second-order and have bounded range of st
ability. The range of stability for the 9-point finite difference scheme is
less restrictive than the (1, 5) FTCS formula. The fully implicit finite d
ifference schemes employed, are based on the (5, 1) backward time centred s
pace (BTCS) formula, and the (5,5) Crank-Nicolson implicit scheme, which ar
e unconditionally stable, but use more CPU times than the fully explicit te
chniques. The basis of analysis of the finite difference equation considere
d here is the modified equivalent partial differential equation approach, d
eveloped from the 1974 work of Warming and Hyeet. This allows direct and si
mple comparison of the eff ors associated with the equations as well as pro
viding a means to develop more accurate finite difference methods. The resu
lts of numerical experiments are presented, and central processor (CPU) tim
es needed for solving this inverse problem are reported.