Theoretical density of the crystal is ρ=nMNoa3 g/cm3
Now, since in Frenkel Defect, there is no change in the theoretical density of the crystal because, in this defect, the only atom switches its position from lattice site to interstitial site.
So, ρ (with 0.1% Frenkel defect) =nMNoa3 g/cm3
a=0.056×10−7 cm ; M=40 g ; n=4 (For FCC)
ρ=40×46.022×1023×(0.056)3×(10−7)3=1.5455 g/cm3
Now, in case of Schottky defect, the density of the crystal changes because the atom leaves the crystal. So, in general for FCC, n=4
But, because o 0.1% Schottky defect, the value of n will change.
So, n′=4–4×0.1100=3.996
ρnew=n′MNoa3=3.996×406.022×1023×(0.556)3×(10−7)3=1.5440 g/cm3