Molybdenum crystallizes in a bcc structure with unit cell dimensions of 0.314 nm. Considering the atomic mass of molybdenum to be 96, its density (in kg $m^{-3}$) is
To find the density ($\rho$) of Molybdenum (Mo) in a body-centered cubic (bcc) structure, we use the formula:
$ \rho = \frac{Z \times M}{V \times N_A} $
Where:
$ V = a^3 = (0.314 \times 10^{-9} \text{ m})^3 $
$ V \approx 0.030959 \times 10^{-27} \text{ m}^3 $
Using the density formula with $Z=2$ for bcc:
$ \rho = \frac{2 \times (96 \times 10^{-3} \text{ kg/mol})}{(0.030959 \times 10^{-27} \text{ m}^3) \times (6.022 \times 10^{23} \text{ mol}^{-1})} $
$ \rho = \frac{0.192}{1.864 \times 10^{-4}} \text{ kg/m}^3 $
$ \rho \approx 10300 \text{ kg/m}^3 $
The calculated density is approximately $10300$ kg/m³, which lies between 10000 and 10500 kg/m³.
The packing efficiency (in %) of spheres for a body-centered cubic (bcc) lattice is approximately
In NaCl crystal, the radius ratio is :
Minimum interplanar spacing required for Bragg’s diffraction is:
What does 'θ' represent in Bragg's Law?
Which of the following is molecular solid?