Thermal properties of magnetically ordered Ce-lattice systems are comp
ared in their crossover to the non-magnetic state, driven by alloying
effects. The ordering temperature (T-ord=T-N or T-C) is found to go to
zero continuously only in a few cases, while in others a discontinuit
y in its decrease is clearly observed. Coincidentally, the magnetic co
ntribution to the specific heat (C-p), the entropy and the free energy
variations with temperature mark an evident difference between those
cases. Furthermore, the extension of the non-fermi-liquid (NFL) phase
in terms of concentration variation correlates with differences observ
ed in the respective ordered phase. A systematic transformation from a
mean field like transition to a fluctuation dominated type is observe
d in C-p(T), as the system overcomes a characteristic crossover concen
tration. Such a concentration appears as a limit for the NFL behavior
in the paramagnetic phase above T-ord. A possible origin of the mentio
ned differences are discussed in terms of some alternatives in the evo
lution of the magnetic moments and the strength of their interactions.