The critical behavior of the two-dimensional Ising model (square latti
ce, exchange constant J) in an uniform field, and in an annealed rando
m field is considered. The random field is generated by decorating the
horizontal and vertical bonds of the lattice, and it satisfies an arb
itrary distribution which is imposed by introducing a pseudo-chemical
potential. By decimating the decorating variables the model can be map
ped onto a homogeneous Ising model with effective exchange constant J'
and effective external field h', dependent on the temperature. These
parameters, which satisfy a set of coupled equations, depend on the sp
in average and nearest-neighbor two-spin correlation, and are obtained
numerically. For the symmetric field distribution p(h(i)) = 1/2[delta
(h + h(i)) + delta(h - h(i))] the mapping of the critical frontier on
the (K' = beta J', H' = beta h') plane onto the (K = beta J, H = beta
h) plane is determined and, as in the model introduced by Essam and Pl
ace, there is a region on the (K, H) plane which cannot be reached fro
m any real values of (K', H'). The critical exponents are determined n
umerically, and it is shown that they do not satisfy renormalization r
elations obtained for their model.