Analyzing the Setup
Let's carefully analyze the geometry of this capacitor
We have a square plate capacitor, separated by a distance d, and the area of each plate is A=L2. The space between the plates is filled with four different dielectrics, K1,K2,K3, and K4.
Because the plates are on the left and right, the electric field goes horizontally. We can think of this system as two parallel branches. The top branch has dielectrics K1 and K2 in series, and the bottom branch has K3 and K4 in series.
Calculating Individual Capacitances
Let's find the capacitance of each individual section
Each section has an area of A/2 and a thickness of d/2.
For the first section,
C1 is given by:
C1=d/2K1ε0(A/2)=dK1ε0A
Similarly, for the other sections, we have:
C2=dK2ε0A
C3=dK3ε0A
C4=dK4ε0A
Series and Parallel Combinations
Since
C1 and
C2 are in series, their equivalent capacitance
C12 is:
C12=C1+C2C1C2=K1+K2K1K2dε0A
By the exact same logic, the bottom branch with
K3 and
K4 in series will have an equivalent capacitance
C34:
C34=C3+C4C3C4=K3+K4K3K4dε0A
Now, these two branches are in parallel. So, the total capacitance
Cnet is simply the sum of
C12 and
C34:
Cnet=C12+C34=(K1+K2K1K2+K3+K4K3K4)dε0A
The Bonus Question Mystery
We equate this Cnet to the capacitance of an equivalent single dielectric K, which is dKε0A
Canceling
dε0A, we find that
K equals:
K=K1+K2K1K2+K3+K4K3K4
Notice that none of the given options match this exact expression, which is why this was a bonus question in the exam!
There is a catch here. What if we inserted a thin conducting foil between the left and right halves? That would force the boundary to be an equipotential surface, putting K1 and K3 in parallel, and K2 and K4 in parallel. If you calculate the effective K for that case, you'll find it matches option (c)! But without that foil, our derived answer is the physically correct one.