  The heavy-fermion metal $\rm CePd_{1-x}Rh_x$ can be tuned from ferromagnetism
at $x=0$ to non-magnetic state at some critical concentration $x_c$. The
non-Fermi liquid behavior (NFL) at $x\simeq x_c$ is recognized by power low
dependence of the specific heat $C(T)$ given by the electronic contribution,
magnetic susceptibility $\chi(T)$ and volume expansion coefficient $\alpha(T)$
at low temperatures: $C/T\propto\chi(T)\propto\alpha(T)/T\propto1/\sqrt{T}$. We
also demonstrate that the behavior of normalized effective mass $M^*_N$
observed in $\rm CePd_{1-x}Rh_x$ at $x\simeq 0.8$ agrees with that of $M^*_N$
observed in paramagnetic $\rm CeRu_2Si_2$ and conclude that these alloys
exhibit the universal NFL thermodynamic behavior at their quantum critical
points. We show that the NFL behavior of $\rm CePd_{1-x}Rh_x$ can be accounted
for within frameworks of quasiparticle picture and fermion condensation quantum
phase transition, while this alloy exhibits a universal thermodynamic NFL
behavior which is independent of the characteristic features of the given alloy
such as its lattice structure, magnetic ground state, dimension etc.
