A metal M crystallizes into two lattices :- face centred cubic (fcc) and body centred cubic (bcc) with unit cell edge length of 20 and \(25 \,\mathring{A}\) respectively The ratio of densities of lattices fcc to bcc for the metal M is ___(Nearest integer)
Remember the formula for density in crystallography: \(\rho = \frac{Z \times M}{N_A \times a^3}\). For fcc, \(Z = 4\); for bcc, \(Z = 2\). Pay close attention to units.
To determine the density ratio of face centred cubic (fcc) to body centred cubic (bcc) lattices of a metal M, we must use formulas for density and unit cell properties.
For a face centred cubic (fcc) lattice:
With edge length \( a = 20 \,\mathring{A} = 20 \times 10^{-8} \) cm, the density becomes:
\(\rho_{\text{fcc}} = \frac{4 \cdot M}{(20 \times 10^{-8})^3 \cdot N_A}\)
For a body centred cubic (bcc) lattice:
With edge length \( a = 25 \,\mathring{A} = 25 \times 10^{-8} \) cm, the density becomes:
\(\rho_{\text{bcc}} = \frac{2 \cdot M}{(25 \times 10^{-8})^3 \cdot N_A}\)
The ratio of densities \( \frac{\rho_{\text{fcc}}}{\rho_{\text{bcc}}} \) is then:
Calculate the values:
Thus, the ratio becomes:
\(\frac{4 \cdot 15625}{2 \cdot 8000} = \frac{62500}{16000} = 3.90625\)
Rounding to the nearest integer gives 4.
Verifying the result, the calculated ratio of 4 lies within the given range [4,4]. Hence, the solution meets the requirements.