Step 1: Understanding the Concept
The upper half, of thickness \(\frac{d}{2}\), has three slabs of area \(\frac{A}{3}\) each side by side, so they are in parallel. The lower half has one dielectric \(k_{4}\) over the full area.
Step 2: Calculation
\(C_{up}=\frac{2\epsilon_{0}A(k_{1}+k_{2}+k_{3})}{3d}\) and \(C_{low}=\frac{2\epsilon_{0}Ak_{4}}{d}\). In series: \(\frac{1}{C}=\frac{3d}{2\epsilon_{0}A(k_{1}+k_{2}+k_{3})}+\frac{d}{2\epsilon_{0}Ak_{4}}\).
Step 3: Compare the options
For one dielectric, \(\frac{1}{C}=\frac{d}{\epsilon_{0}AK}\). Equating and multiplying by \(2\) gives \(\frac{2}{K}=\frac{3}{k_{1}+k_{2}+k_{3}}+\frac{1}{k_{4}}\), the third option.
Final Answer:
The equivalent dielectric constant satisfies \(\frac{2}{k}=\frac{3}{k_{1}+k_{2}+k_{3}}+\frac{1}{k_{4}}\).
\[ \boxed{\text{(C) }\dfrac{2}{k}=\dfrac{3}{k_{1}+k_{2}+k_{3}}+\dfrac{1}{k_{4}}} \]