This solution determines the number density of valence electrons in Sodium (Na) by utilizing its given atomic mass, mass density, and Avogadro's number.
The number density of valence electrons ($n_e$) per unit volume is calculated using the formula:
$n_e = \frac{\text{Density}}{\text{Atomic Mass}} \times \text{Avogadro Number} \times \text{Valence Electrons per Atom}$
Which simplifies to:
$n_e = \frac{\rho}{M} \times N_A \times Z$
$n_{atoms} = \frac{\rho}{M} \times N_A = \frac{0.968 \text{ g cm}^{-3}}{23 \text{ g mol}^{-1}} \times (6.022 \times 10^{23} \text{ mol}^{-1})$
$n_{atoms} \approx 0.042087 \times 6.022 \times 10^{23}$ cm$^{-3}$
$n_{atoms} \approx 0.25345 \times 10^{23}$ atoms cm$^{-3}$
Since each Sodium atom has $1$ valence electron ($Z=1$):
$n_e = n_{atoms} \times Z = (0.25345 \times 10^{23} \text{ cm}^{-3}) \times 1$
$n_e \approx 2.5345 \times 10^{22}$ electrons cm$^{-3}$
The question asks for the value in the format $\_\_\_\_\times 10^{22}$ cm$^{-3}$, rounded to two decimal places.
Rounding $2.5345$ to two decimal places gives $2.53$.
The number density of valence electrons is approximately $2.53$ $\times 10^{22}$ cm$^{-3}$.
Crystal structures of two metals A and B are two-dimensional square lattices with same lattice constant $a$. Electrons in metals behave as free electrons. The Fermi surfaces corresponding to A and B are shown by solid circles in figures. 
The electron concentrations in A and B are $n_A$ and $n_B$, respectively. The value of $(\frac{n_B}{n_A})$ is
If $X$ is the dimensionality of a free electron gas, the energy ($E$) dependence of density of states is given by $E^{½X-Y}$, where $Y$ is ________.