Thermodynamic stabilities of the ordered structures in Pd3Mn have been
theoretically evaluated, both in the presence and absence of hydrogen
. The internal energies of the L1(2) and L1(2-s) structures of Pd3Mn w
ere found to be the same. The L1(2-s) phase is the stable phase at all
temperatures, both in the presence and absence of hydrogen, according
to the statistical thermodynamic calculations indicating that the hyd
rogen-induced ordering phenomenon from the L1(2-s) to the L1(2) struct
ure could be due to stress-assisted motion of atoms as a result of hyd
rogen occupying interstitial sites in the L1(2-s), form. The differenc
e in stabilities between the L1(2) and L1(2-s) structures is small for
both of the cases. The difference in configurational entropies betwee
n the two ordered forms of Pd3Mn decreases with increasing hydrogen co
ncentration. The effect of configurational entropy on the stability of
the L1(2) and L1(2-s) phases has been addressed.