In the strong coupling limit the partition function of SU(2) gauge theory c
an be reduced to that of the continuous spin Ising model with nearest neigh
bour pair-interactions. The random cluster representation of the continuous
spin Ising model in two dimensions is derived through a Fortuin-Kasteleyn
transformation, and the properties of the corresponding cluster distributio
n are analyzed. It is shown that for this model, the magnetic transition is
equivalent to the percolation transition of Fortuin-Kasteleyn clusters, us
ing local bond weights. These results are also illustrated by means of nume
rical simulations. (C) 2000 Elsevier Science B.V. All rights reserved.