[a) = L p Ỵ ^ e - ữ(iM j j - I L P Y jC j , ^ (4) j The first and second derivatives o f the energy o f Eq (4) with respect to a are given by ^ (Ị ) IT—Ị da J jC ^ +2L/ỉaỴ^M je y —ư(ỉA'ỉ j ■) 1Y— I ' -2a-LpỴ^M ]e J —.ơ g M ịt = , and r ">i ( ) J is value o f a for which the lattice is in equilibrium, then energy o f cohesion, [ d ^ l d a \ (5) j ^ = Aa^L(3^YM ]e daAt absolute zero T = 0, a —2,ccoM :r'1 ) gives the is related to the compressibility [1J That IS, (7) where U q{cIq) is the energy o f sublimation at zero pressure and temperature, i,, c., d