Concept:
For heterogeneous equilibria, the activity of a pure solid is taken as unity and does not appear in the equilibrium constant expression.
For the reaction
\[
HgO(s)\rightleftharpoons Hg(g)+\frac12 O_2(g)
\]
\[
K_p=P_{Hg}\,(P_{O_2})^{1/2}
\]
We express the partial pressures in terms of total pressure.
Step 1: Assume decomposition of one mole of HgO.
Let the extent of decomposition be \(x\).
Then
\[
Hg(g)=x
\]
\[
O_2(g)=\frac{x}{2}
\]
Total gaseous moles
\[
n_T=x+\frac{x}{2}
=\frac{3x}{2}
\]
Step 2: Calculate mole fractions.
For mercury vapor,
\[
y_{Hg}
=
\frac{x}{3x/2}
=
\frac{2}{3}
\]
For oxygen,
\[
y_{O_2}
=
\frac{x/2}{3x/2}
=
\frac13
\]
Therefore,
\[
P_{Hg}
=
\frac23 P_T
\]
\[
P_{O_2}
=
\frac13 P_T
\]
Step 3: Substitute into the expression of \(K_p\).
\[
K_p
=
P_{Hg}(P_{O_2})^{1/2}
\]
\[
=
\left(\frac23P_T\right)
\left(\frac13P_T\right)^{1/2}
\]
\[
=
\frac23
\cdot
\frac{1}{\sqrt3}
\cdot
P_T^{3/2}
\]
\[
=
\frac{2}{3\sqrt3}
P_T^{3/2}
\]
\[
=
\frac{2}{3^{3/2}}
P_T^{3/2}
\]
Hence,
\[
\boxed{
K_p=
\frac{2}{3^{3/2}}
P_T^{3/2}
}
\]