Abstract
The renormalization-group transformation, applied earlier to the Hamiltonian Potts model to study the crossover from second-order to first-order transition as the number of states q increases, is extended by taking larger cells in the block transformation. The results improve systematically with increasing block size. The critical value of q above which the transition is of first order, seems to converge to 5 instead of the exactly known value qc=4. The classical equivalents of the new couplings, which drive the system to the first-order transition, are discussed.