Concept:
The capacitance of a parallel plate capacitor filled with a dielectric material is given by \( C = \frac{K \varepsilon_0 A}{d} \).
When capacitors are connected in series to a battery, the electric charge \( Q \) accumulated on their plates is completely identical, which means the potential difference across each capacitor is inversely proportional to its capacitance:
\[
V = \frac{Q}{C} \implies \frac{V_1}{V_2} = \frac{C_2}{C_1}
\]
Step 1: Determining individual capacitance relationships.
Both capacitors share identical structural plate gaps \( d = x \).
• For capacitor \( C_1 \), the dielectric constant is \( K_1 = 3K \implies C_1 \propto 3K \)
• For capacitor \( C_2 \), the dielectric constant is \( K_2 = 6K \implies C_2 \propto 6K \)
Step 2: Calculating the potential difference ratio.
Since they are connected in series across the circuit network loops:
\[
\frac{V_1}{V_2} = \frac{C_2}{C_1} = \frac{6K}{3K} = 2
\]
Thus, the ratio of potential differences is exactly 2.