Step 1: Recall formula for capacitance.
For a parallel plate capacitor with dielectric of thickness $d$ and constant $K$:
\[
C = \frac{\epsilon_0 K A}{d}.
\]
Step 2: Observation of system.
Here, the capacitor contains two dielectric slabs of thicknesses $d_1, d_2$ and constants $K_1, K_2$, placed in series (stacked one after another between plates).
Step 3: Equivalent capacitance for series connection.
For series capacitors:
\[
\frac{1}{C} = \frac{1}{C_1} + \frac{1}{C_2}.
\]
Step 4: Individual capacitances.
\[
C_1 = \frac{\epsilon_0 K_1 A}{d_1},
\quad C_2 = \frac{\epsilon_0 K_2 A}{d_2}.
\]
Step 5: Substitute in series formula.
\[
\frac{1}{C} = \frac{d_1}{\epsilon_0 K_1 A} + \frac{d_2}{\epsilon_0 K_2 A}.
\]
Step 6: Simplify.
\[
\frac{1}{C} = \frac{1}{\epsilon_0 A}\left(\frac{d_1}{K_1} + \frac{d_2}{K_2}\right).
\]
\[
C = \frac{\epsilon_0 A}{\dfrac{d_1}{K_1} + \dfrac{d_2}{K_2}}.
\]
Step 7: Conclusion.
Thus, the capacitance of the system is:
\[
C = \frac{\epsilon_0 A}{\dfrac{d_1}{K_1} + \dfrac{d_2}{K_2}}.
\]