We investigate the probability distribution p(g) of the conductance g in an
isotropic two-dimensional systems. The scaling procedure applicable to mapp
ing the conductance distributions of localized anisotropic systems to the c
orresponding isotropic one can be extended to systems at the critical point
of the metal-to-insulator transition. Instead of the squares used for isot
ropic systems, one should use rectangles for the anisotropic ones. At the c
ritical point, the ratio of the side lengths must be equal to the square ro
ot of the ratio of the critical values of the quasi-one-dimensional scaling
functions. For localized systems, the ratio of the side lengths must be eq
ual to the ratio of the localization lengths.